Acta Physica Sinica - //m.suprmerch.com/ daily 15 2025-03-04 18:10:43 apsoffice@iphy.ac.cn apsoffice@iphy.ac.cn 2025-03-04 18:10:43 zh Copyright ©Acta Physica Sinica All Rights Reserved.  Address: PostCode:100190 Phone: 010-82649829,82649241,82649863 Email: apsoffice@iphy.ac.cn Copyright ©Acta Physica Sinica All Rights Reserved apsoffice@iphy.ac.cn 1000-3290 <![CDATA[The hybrid annealed particle filter]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.999

In this paper, a new particle filter based on sequential importance sampling (SIS) is proposed for the on-line estimation of non-Gaussian nonlinear systems. In this filtering method, state parameters separation and an annealing parameter are used to produce importance function. Since the distribution function makes full use of the prior, likelihood, and statistical characteristics of noise and the newest observation data, it is much closer to posterior distributions. Theoretical analysis and simulation show that the performance of proposed particle filter outperforms the standard particle filter and the extended Kalman filter.


Acta Physica Sinica. 2006 55(3): 999-1004. Published 2006-03-20 ]]>

In this paper, a new particle filter based on sequential importance sampling (SIS) is proposed for the on-line estimation of non-Gaussian nonlinear systems. In this filtering method, state parameters separation and an annealing parameter are used to produce importance function. Since the distribution function makes full use of the prior, likelihood, and statistical characteristics of noise and the newest observation data, it is much closer to posterior distributions. Theoretical analysis and simulation show that the performance of proposed particle filter outperforms the standard particle filter and the extended Kalman filter.


Acta Physica Sinica. 2006 55(3): 999-1004. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 999-1004. article doi:10.7498/aps.55.999 10.7498/aps.55.999 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.999 999-1004
<![CDATA[A numerical method for two-phase flow in micro channels and its application to droplet control by electrowetting on dielectric]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1005

With the development of micro chemical and medical analysis in MEMS, micro-fluid-control chip becomes more and more popular. Based on discrete droplet control system, chemical and medical analysis is applied in the micro chip lab. The change of voltage between the dielectric layer of the electrode controls the wettability of a droplet on a dielectric solid surface and then makes it possible to create,transport,merge and cut the micro droplets. This paper presents a numerical method to simulate the droplet motion by electrowetting on dielectric (EWOD). The second-order projection method is carried out to solve N-S equations and level set function. The interface is captured as zero level set. Dynamic contact angle for fluid contacting a solid surface by the electric potential is used to evaluate the wettability of fluid by EWOD. The numerical scheme is based on staggered MAC grid. Numerical simulations are used to capture the interface between two kinds of fluids in micro channels, the shapes of micro droplets resting on the horizontal solid surface under different electric potential and the transportation of a micro droplet in a parallel-plate channel when electrodes are activated.


Acta Physica Sinica. 2006 55(3): 1005-1010. Published 2006-03-20 ]]>

With the development of micro chemical and medical analysis in MEMS, micro-fluid-control chip becomes more and more popular. Based on discrete droplet control system, chemical and medical analysis is applied in the micro chip lab. The change of voltage between the dielectric layer of the electrode controls the wettability of a droplet on a dielectric solid surface and then makes it possible to create,transport,merge and cut the micro droplets. This paper presents a numerical method to simulate the droplet motion by electrowetting on dielectric (EWOD). The second-order projection method is carried out to solve N-S equations and level set function. The interface is captured as zero level set. Dynamic contact angle for fluid contacting a solid surface by the electric potential is used to evaluate the wettability of fluid by EWOD. The numerical scheme is based on staggered MAC grid. Numerical simulations are used to capture the interface between two kinds of fluids in micro channels, the shapes of micro droplets resting on the horizontal solid surface under different electric potential and the transportation of a micro droplet in a parallel-plate channel when electrodes are activated.


Acta Physica Sinica. 2006 55(3): 1005-1010. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1005-1010. article doi:10.7498/aps.55.1005 10.7498/aps.55.1005 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1005 1005-1010
<![CDATA[General multi-linear variable separation approach to solving low dimensional nonlinear systems and localized exitations]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1011

Multi-linear variable separation approach based on the corresponding Bcklund transformation (BT-MLVSA) is a useful method to solve nonlinear systems. General multi-linear variable separation approach (GMLVSA) is its extension and there are four ways to realize it. The first one is to expand the nonlinear systems according to multi-arbitrary functions, the second one is to expand the variable separation ansatz. The third one is the MLVSA based on the Darboux transformation (DT-MLVSA) and the last one is the derivative-dependent functional variable separation method. By using the first kind of GMLVSA, the solutions can be obtained for the (2+1)-dimensional mNNV system and sine-Gordon system. In this paper, the first kind of GMLVSA is extended to solve some two-dimensional nonlinear systems which are derived from the (2+1)-dimensional sine-Gordon system by using symmetry reduction method. Namely, the applicability of the method is retained from high dimensional systems to low dimensional systems in the symmery reduction sense. This also provide a way of deducing low dimensional systems which can be solved by GMLVSA from high dimensional systems.


Acta Physica Sinica. 2006 55(3): 1011-1015. Published 2006-03-20 ]]>

Multi-linear variable separation approach based on the corresponding Bcklund transformation (BT-MLVSA) is a useful method to solve nonlinear systems. General multi-linear variable separation approach (GMLVSA) is its extension and there are four ways to realize it. The first one is to expand the nonlinear systems according to multi-arbitrary functions, the second one is to expand the variable separation ansatz. The third one is the MLVSA based on the Darboux transformation (DT-MLVSA) and the last one is the derivative-dependent functional variable separation method. By using the first kind of GMLVSA, the solutions can be obtained for the (2+1)-dimensional mNNV system and sine-Gordon system. In this paper, the first kind of GMLVSA is extended to solve some two-dimensional nonlinear systems which are derived from the (2+1)-dimensional sine-Gordon system by using symmetry reduction method. Namely, the applicability of the method is retained from high dimensional systems to low dimensional systems in the symmery reduction sense. This also provide a way of deducing low dimensional systems which can be solved by GMLVSA from high dimensional systems.


Acta Physica Sinica. 2006 55(3): 1011-1015. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1011-1015. article doi:10.7498/aps.55.1011 10.7498/aps.55.1011 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1011 1011-1015
<![CDATA[Variable separation solution and soliton excitations of the (1+1)-dimensional generalised shallow water wave equation]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1016

In this paper, variable separation solution and soliton excitations of the (1+1)-dimensional generalised shallow water wave equation are obtained. This equation includes two special cases which are completely integrable (IST integrable): the AKNS equation and the Hirota-Satsuma equation. Firstly, the variable separation (BT-VS) method based on the Bcklund transformation is extended to this eqaution for deriving VS solutions which include some low dimensional arbitrary functions. In the integrable cases, a space arbitrary function and a time arbitrary function are included. But in the other cases only a time arbitrary function is included and the space function needs to satisfy a specific condition. In addition, for the (1+1)-dimensional universal formula, abundant soliton excitations can be constructed, such as one-soliton, bell-anti-bell soltion, soliton expansion, breather-like, instaton-like. Finally, some discusions are made about the VT-VS method.


Acta Physica Sinica. 2006 55(3): 1016-1022. Published 2006-03-20 ]]>

In this paper, variable separation solution and soliton excitations of the (1+1)-dimensional generalised shallow water wave equation are obtained. This equation includes two special cases which are completely integrable (IST integrable): the AKNS equation and the Hirota-Satsuma equation. Firstly, the variable separation (BT-VS) method based on the Bcklund transformation is extended to this eqaution for deriving VS solutions which include some low dimensional arbitrary functions. In the integrable cases, a space arbitrary function and a time arbitrary function are included. But in the other cases only a time arbitrary function is included and the space function needs to satisfy a specific condition. In addition, for the (1+1)-dimensional universal formula, abundant soliton excitations can be constructed, such as one-soliton, bell-anti-bell soltion, soliton expansion, breather-like, instaton-like. Finally, some discusions are made about the VT-VS method.


Acta Physica Sinica. 2006 55(3): 1016-1022. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1016-1022. article doi:10.7498/aps.55.1016 10.7498/aps.55.1016 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1016 1016-1022
<![CDATA[A highly efficient beam propagation method for modeling step-index waveguides with tilt interface]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1023

Based on a new finite-difference scheme and Runge-Kutta method together with transparent boundary conditions(TBCs), a novel beam propagation method to model step-index waveguides with tilt interfaces is presented. The modified scheme provides an precies description of the tilt interface of the nonrectangular waveguide structure, showing a much better efficiency and accuracy comparing with the previously presented formulas.


Acta Physica Sinica. 2006 55(3): 1023-1028. Published 2006-03-20 ]]>

Based on a new finite-difference scheme and Runge-Kutta method together with transparent boundary conditions(TBCs), a novel beam propagation method to model step-index waveguides with tilt interfaces is presented. The modified scheme provides an precies description of the tilt interface of the nonrectangular waveguide structure, showing a much better efficiency and accuracy comparing with the previously presented formulas.


Acta Physica Sinica. 2006 55(3): 1023-1028. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1023-1028. article doi:10.7498/aps.55.1023 10.7498/aps.55.1023 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1023 1023-1028
<![CDATA[Solitary wave solution of Zakharov equation with quantum effect]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1029

With the help of Maple procedure, the Zakharov equation, which takes the quantum effect into account, is solved by means of extended tanh-function method and bifunction method. Several solitary wave solutions are obtained, including bright soliton, W-shaped soliton, M-shaped soliton and singular solutions.


Acta Physica Sinica. 2006 55(3): 1029-1034. Published 2006-03-20 ]]>

With the help of Maple procedure, the Zakharov equation, which takes the quantum effect into account, is solved by means of extended tanh-function method and bifunction method. Several solitary wave solutions are obtained, including bright soliton, W-shaped soliton, M-shaped soliton and singular solutions.


Acta Physica Sinica. 2006 55(3): 1029-1034. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1029-1034. article doi:10.7498/aps.55.1029 10.7498/aps.55.1029 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1029 1029-1034
<![CDATA[Chaos synchronization between the Sprott-B and Sprott-C with linear coupling]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1035

The Sprott-B and Sprott-C are topologically equivalent but they have distinct structures. Chaos synchronization is realized between the two systems via linear coupling of systemic variable. Based on Lyapunov stability theory, the threshold value of coupling coefficients for synchronization of two systems is derived. The practical circuit is designed to realize chaos synchronization between the two systems and the experimental result verifies the conclusion. A new method for secure communication, which can increase the security of a communication system is proposed based on chaos synchronization between the above systems.


Acta Physica Sinica. 2006 55(3): 1035-1039. Published 2006-03-20 ]]>

The Sprott-B and Sprott-C are topologically equivalent but they have distinct structures. Chaos synchronization is realized between the two systems via linear coupling of systemic variable. Based on Lyapunov stability theory, the threshold value of coupling coefficients for synchronization of two systems is derived. The practical circuit is designed to realize chaos synchronization between the two systems and the experimental result verifies the conclusion. A new method for secure communication, which can increase the security of a communication system is proposed based on chaos synchronization between the above systems.


Acta Physica Sinica. 2006 55(3): 1035-1039. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1035-1039. article doi:10.7498/aps.55.1035 10.7498/aps.55.1035 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1035 1035-1039
<![CDATA[Study on the delayed feedback control of chaos in chaotic neural networks]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1040

Chaotic neural networks consisting of chaotic neurons exhibit rich dynamic behaviors and are expected to be used in information processing. But the output sequence of chaotic neural networks is chaotic, so the networks do not converge to a stable pattern. In order to apply chaotic neural networks to information search or pattern recognition, etc., it is necessary to control chaos in chaotic neural networks. In this paper, we propose an improved delayed feedback control method for chaotic neural networks. By means of the control method, computer simulation shows that controlled chaotic neural networks can converge to period-2 states between one stored pattern and its reverse pattern or various multiple-period states depending on the delay time.


Acta Physica Sinica. 2006 55(3): 1040-1048. Published 2006-03-20 ]]>

Chaotic neural networks consisting of chaotic neurons exhibit rich dynamic behaviors and are expected to be used in information processing. But the output sequence of chaotic neural networks is chaotic, so the networks do not converge to a stable pattern. In order to apply chaotic neural networks to information search or pattern recognition, etc., it is necessary to control chaos in chaotic neural networks. In this paper, we propose an improved delayed feedback control method for chaotic neural networks. By means of the control method, computer simulation shows that controlled chaotic neural networks can converge to period-2 states between one stored pattern and its reverse pattern or various multiple-period states depending on the delay time.


Acta Physica Sinica. 2006 55(3): 1040-1048. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1040-1048. article doi:10.7498/aps.55.1040 10.7498/aps.55.1040 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1040 1040-1048
<![CDATA[Chaos control of Duffing systems by random phase]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1049

In this paper, the effect of random phase for Duffing systems is investigated. We show that random phase can generate chaos or suppress chaos by the average of top Lyapunov exponent, which is computed based on Khasminskii's spherical coordinate formulation for linear stochastic systems. In addition, phase portraits, Poincaré surface of section and time evolution are studied to confirm the obtained results. Both methods lead to fully consistent results.


Acta Physica Sinica. 2006 55(3): 1049-1054. Published 2006-03-20 ]]>

In this paper, the effect of random phase for Duffing systems is investigated. We show that random phase can generate chaos or suppress chaos by the average of top Lyapunov exponent, which is computed based on Khasminskii's spherical coordinate formulation for linear stochastic systems. In addition, phase portraits, Poincaré surface of section and time evolution are studied to confirm the obtained results. Both methods lead to fully consistent results.


Acta Physica Sinica. 2006 55(3): 1049-1054. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1049-1054. article doi:10.7498/aps.55.1049 10.7498/aps.55.1049 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1049 1049-1054
<![CDATA[Determination of anisotropic liquid crystal layer parameters by spectroscopic ellipsometer]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1055

Spectroscopic ellipsometry is widely used in measuring the refractive index and thickness of optical isotropic thin layers. A simple method using spectroscopic ellipsometry to measure uniaxial liquid crystal layer is introduced. A UVISEL spectroscopic phase modulated ellipsometer is used to measure the ordinary refractive index, extraordinary refractive index and thickness of the liquid crystal layer in a parallel-aligned liquid crystal cell. The phase retardation Δnd is measured in transmission mode. The results show that the spectroscopic ellipsometry can be used to measure the anisotropic multilayer liquid crystal cell with high precision.


Acta Physica Sinica. 2006 55(3): 1055-1060. Published 2006-03-20 ]]>

Spectroscopic ellipsometry is widely used in measuring the refractive index and thickness of optical isotropic thin layers. A simple method using spectroscopic ellipsometry to measure uniaxial liquid crystal layer is introduced. A UVISEL spectroscopic phase modulated ellipsometer is used to measure the ordinary refractive index, extraordinary refractive index and thickness of the liquid crystal layer in a parallel-aligned liquid crystal cell. The phase retardation Δnd is measured in transmission mode. The results show that the spectroscopic ellipsometry can be used to measure the anisotropic multilayer liquid crystal cell with high precision.


Acta Physica Sinica. 2006 55(3): 1055-1060. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1055-1060. article doi:10.7498/aps.55.1055 10.7498/aps.55.1055 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1055 1055-1060
<![CDATA[Effect of polarization of THz pulse and probe pulse on THz electro-optic detection]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1061

We studied the effect of polarization of terahertz pulse and probe beam on terahertz detection in optically isotropic detection crystals using wave coupling theory of linear electro-optic effect. The study results show that the effect is remarkable, and the detection can get its largest sensitivity when the probe beam propagates along (110) direction which is most suitable for terahertz detection. Some of the study results are in good agreement with the previously published experimental results. So our study is helpful for the design of electro-optic detectors.


Acta Physica Sinica. 2006 55(3): 1061-1067. Published 2006-03-20 ]]>

We studied the effect of polarization of terahertz pulse and probe beam on terahertz detection in optically isotropic detection crystals using wave coupling theory of linear electro-optic effect. The study results show that the effect is remarkable, and the detection can get its largest sensitivity when the probe beam propagates along (110) direction which is most suitable for terahertz detection. Some of the study results are in good agreement with the previously published experimental results. So our study is helpful for the design of electro-optic detectors.


Acta Physica Sinica. 2006 55(3): 1061-1067. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1061-1067. article doi:10.7498/aps.55.1061 10.7498/aps.55.1061 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1061 1061-1067
<![CDATA[Nuclear reaction dynamics induced by halo-nuclei at intermediate energy heavy ion collisions]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1068

We studied systematically the reaction dynamics induced by neutron-halo nuclei and proton-halo nuclei within the isospin dependent quantum molecular dynamics,such as the effects of loose bound halo-nuclei on the fragmentation reaction and momentum dissipation for different colliding systems with different beam energies and different impact parameters. In order to emphasize the roles of neutron-halo nucleus 19B and proton-halo nucleus 23Al on the reaction dynamics wealso calculated the the reaction dynamics induced by the stable nuclei 19F and 23Na with equal mass under identical incident channel conditions. Based on the comparison of results of reaction dynamics induced by halo-nucleus colliding systems and stable nucleus collidinmg systems we found that the roles of loose bound halo-nucleus structure on the fragmentation multiplicity and nuclear stopping (momentum dissipation) are important for all of colliding systems with different beam energies and minor impact parameters, such as, the loose bound halo-nuclei structure increases the fragmentation multiplicity, but reduces the nuclear stopping.


Acta Physica Sinica. 2006 55(3): 1068-1076. Published 2006-03-20 ]]>

We studied systematically the reaction dynamics induced by neutron-halo nuclei and proton-halo nuclei within the isospin dependent quantum molecular dynamics,such as the effects of loose bound halo-nuclei on the fragmentation reaction and momentum dissipation for different colliding systems with different beam energies and different impact parameters. In order to emphasize the roles of neutron-halo nucleus 19B and proton-halo nucleus 23Al on the reaction dynamics wealso calculated the the reaction dynamics induced by the stable nuclei 19F and 23Na with equal mass under identical incident channel conditions. Based on the comparison of results of reaction dynamics induced by halo-nucleus colliding systems and stable nucleus collidinmg systems we found that the roles of loose bound halo-nucleus structure on the fragmentation multiplicity and nuclear stopping (momentum dissipation) are important for all of colliding systems with different beam energies and minor impact parameters, such as, the loose bound halo-nuclei structure increases the fragmentation multiplicity, but reduces the nuclear stopping.


Acta Physica Sinica. 2006 55(3): 1068-1076. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1068-1076. article doi:10.7498/aps.55.1068 10.7498/aps.55.1068 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1068 1068-1076
<![CDATA[Confinement of fast ions in east tokamak]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1077

The three well-known parameters of motion (magnetic momentum, energy and canonical toroidal momentum) are utilized to develop a guiding center orbit code, GCORBIT. The effect of poroidal field ripple and toroidal angle scatter is considered in the GCORBIT. It is applied to compute guiding center orbit of charged particle in axisymmetric tokamak, the loss region of velocity space and the loss fraction of fast ions.To compare achieved results, the loss region of velocity space by GCORBIT includes many effects: non-closed orbit of divertor, first orbit loss by guiding-center orbit being non-closed or intersecting with any material limiters, trapping by the poroidal field ripple in local magnetic wells, ripple random diffusion and toroidal angle scatter enabled by velocity space discontinuous confinement region. The GCORBIT is now being used to analyze the confinement of fast ions in EAST Tokamak. Our numerical calculations are focused on the loss of fast ions.


Acta Physica Sinica. 2006 55(3): 1077-1082. Published 2006-03-20 ]]>

The three well-known parameters of motion (magnetic momentum, energy and canonical toroidal momentum) are utilized to develop a guiding center orbit code, GCORBIT. The effect of poroidal field ripple and toroidal angle scatter is considered in the GCORBIT. It is applied to compute guiding center orbit of charged particle in axisymmetric tokamak, the loss region of velocity space and the loss fraction of fast ions.To compare achieved results, the loss region of velocity space by GCORBIT includes many effects: non-closed orbit of divertor, first orbit loss by guiding-center orbit being non-closed or intersecting with any material limiters, trapping by the poroidal field ripple in local magnetic wells, ripple random diffusion and toroidal angle scatter enabled by velocity space discontinuous confinement region. The GCORBIT is now being used to analyze the confinement of fast ions in EAST Tokamak. Our numerical calculations are focused on the loss of fast ions.


Acta Physica Sinica. 2006 55(3): 1077-1082. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1077-1082. article doi:10.7498/aps.55.1077 10.7498/aps.55.1077 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1077 1077-1082
<![CDATA[Photoionization and dissociative photoionization study of HFC-152a using synchrotron radiation]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1083

Photoionization and dissociative photoionization of HFC-152a have been studied using synchrotron radiation and a reflectron time-of-flight mass spectrometry (RTOF-MS). The ionization energy of parent molecule (11.94±0.04eV) and appearance potentials of various fragment ions have been determined by measuring their photoionization efficiency curves. Energies, symmetry point groups and ground electronic states of neutrals and cations of parent and its fragments have been calculated using GAUSSIAN-03 program with the G3 method. According to the theoretical and experimental results, some dissociation channels and their dissociation energies of CH3CHF+2 have been analyzed.


Acta Physica Sinica. 2006 55(3): 1083-1088. Published 2006-03-20 ]]>

Photoionization and dissociative photoionization of HFC-152a have been studied using synchrotron radiation and a reflectron time-of-flight mass spectrometry (RTOF-MS). The ionization energy of parent molecule (11.94±0.04eV) and appearance potentials of various fragment ions have been determined by measuring their photoionization efficiency curves. Energies, symmetry point groups and ground electronic states of neutrals and cations of parent and its fragments have been calculated using GAUSSIAN-03 program with the G3 method. According to the theoretical and experimental results, some dissociation channels and their dissociation energies of CH3CHF+2 have been analyzed.


Acta Physica Sinica. 2006 55(3): 1083-1088. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1083-1088. article doi:10.7498/aps.55.1083 10.7498/aps.55.1083 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1083 1083-1088
<![CDATA[Principles of X-ray diffraction enhanced imaging]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1089

The interactions between X-ray and the sample and crystals were investigated, and the influence of small angle scattering on images was emphatically analyzed in diffraction enhanced imaging in this paper. Not only were the additional noise term caused by small angle scattering introduced, and more general DEI equation established, but also expressions of absorption contrast, extinction contrast and refraction contrast were given for the peak image and the middle slope image. With the new DEI equation, the contrasts of two kinds of resultant images (apparent absorption image and refraction image) were discussed.


Acta Physica Sinica. 2006 55(3): 1089-1098. Published 2006-03-20 ]]>

The interactions between X-ray and the sample and crystals were investigated, and the influence of small angle scattering on images was emphatically analyzed in diffraction enhanced imaging in this paper. Not only were the additional noise term caused by small angle scattering introduced, and more general DEI equation established, but also expressions of absorption contrast, extinction contrast and refraction contrast were given for the peak image and the middle slope image. With the new DEI equation, the contrasts of two kinds of resultant images (apparent absorption image and refraction image) were discussed.


Acta Physica Sinica. 2006 55(3): 1089-1098. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1089-1098. article doi:10.7498/aps.55.1089 10.7498/aps.55.1089 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1089 1089-1098
<![CDATA[Diffraction enhanced imaging computer tomography]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1099

Diffraction enhanced imaging is a new X-ray radiographic imaging method using monochromatic X-rays from a synchrotron source which produces high contrast and spatial resolution images of thick absorbing objects. Use of this method in medicine, material science and industrial applications in non-destructive testing is highlighted at present. The purpose of this study is to discuss diffraction enhanced imaging computer tomography which combines computer tomography (CT) and diffraction enhanced imaging (DEI) method. Comparison between DEI-CT images with conventional X-ray CT images shows that the DEI-CT imaging technique gives not only surface information but also the internal structure of organs or soft tissues with high contrast. The obtained images show the micro-structures details of DEI-CT.


Acta Physica Sinica. 2006 55(3): 1099-1106. Published 2006-03-20 ]]>

Diffraction enhanced imaging is a new X-ray radiographic imaging method using monochromatic X-rays from a synchrotron source which produces high contrast and spatial resolution images of thick absorbing objects. Use of this method in medicine, material science and industrial applications in non-destructive testing is highlighted at present. The purpose of this study is to discuss diffraction enhanced imaging computer tomography which combines computer tomography (CT) and diffraction enhanced imaging (DEI) method. Comparison between DEI-CT images with conventional X-ray CT images shows that the DEI-CT imaging technique gives not only surface information but also the internal structure of organs or soft tissues with high contrast. The obtained images show the micro-structures details of DEI-CT.


Acta Physica Sinica. 2006 55(3): 1099-1106. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1099-1106. article doi:10.7498/aps.55.1099 10.7498/aps.55.1099 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1099 1099-1106
<![CDATA[Molecular dynamics modelling of adsorption of HEDP on calcite surface]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1107

The molecular dynamics modeling method is used to study the adsorption characteristics of 1-hydroxyethyldene-1,1-diphosphonic acid(HEDP) on the {104} surface of calcite. The simulated 3-D molecular graphs display that the oxygen atoms in the phosphonate groups of HEDP are strongly electro negative and have high affinity to cationic regions of the surface of the crystals, which results in the inhibitor molecular binding to the crystal surface to form the “multi-site stereo matching'. The calculated results show that the adsorption energy of HEDP on the surface, step and kink are -5.2eV,-7.0eV and -23.5eV, respectively. It suggestes that HEDP malecules prefer to adsorb on the kinks to inhibit the development of steps on the calcite surface.


Acta Physica Sinica. 2006 55(3): 1107-1112. Published 2006-03-20 ]]>

The molecular dynamics modeling method is used to study the adsorption characteristics of 1-hydroxyethyldene-1,1-diphosphonic acid(HEDP) on the {104} surface of calcite. The simulated 3-D molecular graphs display that the oxygen atoms in the phosphonate groups of HEDP are strongly electro negative and have high affinity to cationic regions of the surface of the crystals, which results in the inhibitor molecular binding to the crystal surface to form the “multi-site stereo matching'. The calculated results show that the adsorption energy of HEDP on the surface, step and kink are -5.2eV,-7.0eV and -23.5eV, respectively. It suggestes that HEDP malecules prefer to adsorb on the kinks to inhibit the development of steps on the calcite surface.


Acta Physica Sinica. 2006 55(3): 1107-1112. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1107-1112. article doi:10.7498/aps.55.1107 10.7498/aps.55.1107 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1107 1107-1112
<![CDATA[Study on the structure and stability of the AlxOy(x=1—2,y=1—3) molecules by deusity function theory]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1113

The geometric configuration, electronic structures and vibrational frequency of the AlxOy(x=1—2,y=1—3) molecules were calculated with B3LYP method at 6-311++g** level. The calculations show that the ground states of AlxOy molecules can be rapidly obtained by adding one or two O atoms to the different positions of Oy clusters with the aid of the software Gaussview 3.7, and taking into account of possible symmetries. Analysis of the geometrical parameters of ground state structure reveals that the atoms have chained or planar structure only. Analysis of the energy of ground state structure shows that Al atoms tend to bind with three other atoms. With one Al atom in the molecule the ground state structures multiplicity is two, with two Al atoms in the molecule, the ground state structures multiplicity is one except for Al2O3, of which the ground state structures multiplicity is three.


Acta Physica Sinica. 2006 55(3): 1113-1118. Published 2006-03-20 ]]>

The geometric configuration, electronic structures and vibrational frequency of the AlxOy(x=1—2,y=1—3) molecules were calculated with B3LYP method at 6-311++g** level. The calculations show that the ground states of AlxOy molecules can be rapidly obtained by adding one or two O atoms to the different positions of Oy clusters with the aid of the software Gaussview 3.7, and taking into account of possible symmetries. Analysis of the geometrical parameters of ground state structure reveals that the atoms have chained or planar structure only. Analysis of the energy of ground state structure shows that Al atoms tend to bind with three other atoms. With one Al atom in the molecule the ground state structures multiplicity is two, with two Al atoms in the molecule, the ground state structures multiplicity is one except for Al2O3, of which the ground state structures multiplicity is three.


Acta Physica Sinica. 2006 55(3): 1113-1118. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1113-1118. article doi:10.7498/aps.55.1113 10.7498/aps.55.1113 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1113 1113-1118
<![CDATA[Numerical calculation of multiple scattering of high frequency electromagnetic wave]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1119

Using physical optics to calculate single scattering, and using equivalent ray tubes to calculate multiple scattering, we can get the numerical results more efficiently and accurately. Several complex perfect electric conductors and medium targets are calculated, and numerical results are in good agreement with experiments.


Acta Physica Sinica. 2006 55(3): 1119-1125. Published 2006-03-20 ]]>

Using physical optics to calculate single scattering, and using equivalent ray tubes to calculate multiple scattering, we can get the numerical results more efficiently and accurately. Several complex perfect electric conductors and medium targets are calculated, and numerical results are in good agreement with experiments.


Acta Physica Sinica. 2006 55(3): 1119-1125. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1119-1125. article doi:10.7498/aps.55.1119 10.7498/aps.55.1119 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1119 1119-1125
<![CDATA[Design of an improved Fresnel prism]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1126

Based on the optimization of the optical material and internal reflection angle, we designed a model of improved Fresnel prism that is insensitive to the angle of incidence. In this device, the incident light is reflected twice at the same internal reflection angle on the interface between two kinds of glass and the air. So the changes of retardation caused by reflection can compensate each other. The calculation shows that the departure of this kind of phase retarders is less than 0.36° when the angle of incidence changes between -2° and +2°.It reserves the merits of normal incidence and normal output in archetypal Fresnel prism, and brings convenience in the operation.


Acta Physica Sinica. 2006 55(3): 1126-1129. Published 2006-03-20 ]]>

Based on the optimization of the optical material and internal reflection angle, we designed a model of improved Fresnel prism that is insensitive to the angle of incidence. In this device, the incident light is reflected twice at the same internal reflection angle on the interface between two kinds of glass and the air. So the changes of retardation caused by reflection can compensate each other. The calculation shows that the departure of this kind of phase retarders is less than 0.36° when the angle of incidence changes between -2° and +2°.It reserves the merits of normal incidence and normal output in archetypal Fresnel prism, and brings convenience in the operation.


Acta Physica Sinica. 2006 55(3): 1126-1129. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1126-1129. article doi:10.7498/aps.55.1126 10.7498/aps.55.1126 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1126 1126-1129
<![CDATA[Known-plaintext attack on double phase encoding encryption technique]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1130

In the field of optical information security, the most attractive work is the so-called double-random-phase encoding encryption scheme proposed by Javidi. However, the security of this cryptosystem has not been analyzed thoroughly from the point of view of cryptoanalysis. In this article, the weakness of Javidi's optical security system is carefully analyzed with a known-plain text attack. It is shown that the double-random-phase encoding encryption scheme is a linear symmetric block cipher cryptosystem and its linearity opens avenues of attacks. Under the known-plaintext attack, attacker can obtain the phase key(s) in the input plane using the typical phase retrieval algorithms and subsequently deduce the phase key(s) in the Fourier domain easily. In addition, an optical implementation of known-plain text attack is also proposed.


Acta Physica Sinica. 2006 55(3): 1130-1136. Published 2006-03-20 ]]>

In the field of optical information security, the most attractive work is the so-called double-random-phase encoding encryption scheme proposed by Javidi. However, the security of this cryptosystem has not been analyzed thoroughly from the point of view of cryptoanalysis. In this article, the weakness of Javidi's optical security system is carefully analyzed with a known-plain text attack. It is shown that the double-random-phase encoding encryption scheme is a linear symmetric block cipher cryptosystem and its linearity opens avenues of attacks. Under the known-plaintext attack, attacker can obtain the phase key(s) in the input plane using the typical phase retrieval algorithms and subsequently deduce the phase key(s) in the Fourier domain easily. In addition, an optical implementation of known-plain text attack is also proposed.


Acta Physica Sinica. 2006 55(3): 1130-1136. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1130-1136. article doi:10.7498/aps.55.1130 10.7498/aps.55.1130 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1130 1130-1136
<![CDATA[Spatially angular multiplexing in ultra-short pulsed digital holography]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1137

Ultra-fast dynamic process can be recorded by ultra-short pulsed digital holography with angular multiplexing technique, in which the angle between reference beam and object beam has to be restricted to within a few degrees due to the restricted pixel size of CCD in the recording. In this report, spatially angular multiplexing technique is introduced, and the its applicability has been proved through a simulation experiment of digital holography with CW laser. Besides, optical set-up based on this technique is designed. Computation result shows that a series of dynamic multi-images in nanosecond time scale of ultra-fast process can be automatically recorded on a piece of digital hologram.


Acta Physica Sinica. 2006 55(3): 1137-1142. Published 2006-03-20 ]]>

Ultra-fast dynamic process can be recorded by ultra-short pulsed digital holography with angular multiplexing technique, in which the angle between reference beam and object beam has to be restricted to within a few degrees due to the restricted pixel size of CCD in the recording. In this report, spatially angular multiplexing technique is introduced, and the its applicability has been proved through a simulation experiment of digital holography with CW laser. Besides, optical set-up based on this technique is designed. Computation result shows that a series of dynamic multi-images in nanosecond time scale of ultra-fast process can be automatically recorded on a piece of digital hologram.


Acta Physica Sinica. 2006 55(3): 1137-1142. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1137-1142. article doi:10.7498/aps.55.1137 10.7498/aps.55.1137 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1137 1137-1142
<![CDATA[Design of multi-layer dielectric grating for femtosecond laser]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1143

Based on optical interference theory and Fourier modal theory, a new multi-layer dielectric gratings is designed for use in femtosecond laser system at wavelength 0.8μm. A multi-layer dielectric with stack of H3L(HL)^9H0.5L2.4H is used as a substrate to be etched with corrugated structure. Numerical computation indicates that the diffraction efficiency of -1 order can be more than 95% when the parameters of multi-layer dielectric grating are the following: laser is incident on the grating at 36.7° in TE mode, the duty cycle is 0.35 and the line density is 1480/mm, the groove depth is 0.2μm and the top residual HfO2 is 0.15μm.


Acta Physica Sinica. 2006 55(3): 1143-1147. Published 2006-03-20 ]]>

Based on optical interference theory and Fourier modal theory, a new multi-layer dielectric gratings is designed for use in femtosecond laser system at wavelength 0.8μm. A multi-layer dielectric with stack of H3L(HL)^9H0.5L2.4H is used as a substrate to be etched with corrugated structure. Numerical computation indicates that the diffraction efficiency of -1 order can be more than 95% when the parameters of multi-layer dielectric grating are the following: laser is incident on the grating at 36.7° in TE mode, the duty cycle is 0.35 and the line density is 1480/mm, the groove depth is 0.2μm and the top residual HfO2 is 0.15μm.


Acta Physica Sinica. 2006 55(3): 1143-1147. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1143-1147. article doi:10.7498/aps.55.1143 10.7498/aps.55.1143 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1143 1143-1147
<![CDATA[Electron holography investigation of the barrier of magnetic tunnelling junctions]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1148

Electron holography was successfully used to investigate the distribution of the potential of the barrier in magnetic tunnelling junctions experimentally and theoretically. We got a clear profile of the potential which shows a “well” in reconstructed phase profile. We also pointed out some artefacts in electron holographic study of magnetic tunnelling junctions and suggested some possible methods to resolve them.


Acta Physica Sinica. 2006 55(3): 1148-1152. Published 2006-03-20 ]]>

Electron holography was successfully used to investigate the distribution of the potential of the barrier in magnetic tunnelling junctions experimentally and theoretically. We got a clear profile of the potential which shows a “well” in reconstructed phase profile. We also pointed out some artefacts in electron holographic study of magnetic tunnelling junctions and suggested some possible methods to resolve them.


Acta Physica Sinica. 2006 55(3): 1148-1152. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1148-1152. article doi:10.7498/aps.55.1148 10.7498/aps.55.1148 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1148 1148-1152
<![CDATA[Resonant tunneling and photon emission of an ultracold two-level atom passing through multi single-mode cavity fields]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1153

We consider that an ultracold two-level atom passes through multi spatially separated single-mode cavity fields and investigate the influence of the center-of-mass motion of the atom, the length of the cavity and the separation between two cavities on the transmission and photon emission probabilities of the atom. We find that both the transmission and photon emission probabilities as functions of the cavity length have multi-resonance peaks when the separation between two cavities is equal to an integer multiple of half the de Broglie wavelength of the atomic center-of-mass motion. The present work shows that the wave function of the atomic center-of-mass motion may be modulated in a macroscopic level by arranging the cavities.


Acta Physica Sinica. 2006 55(3): 1153-1159. Published 2006-03-20 ]]>

We consider that an ultracold two-level atom passes through multi spatially separated single-mode cavity fields and investigate the influence of the center-of-mass motion of the atom, the length of the cavity and the separation between two cavities on the transmission and photon emission probabilities of the atom. We find that both the transmission and photon emission probabilities as functions of the cavity length have multi-resonance peaks when the separation between two cavities is equal to an integer multiple of half the de Broglie wavelength of the atomic center-of-mass motion. The present work shows that the wave function of the atomic center-of-mass motion may be modulated in a macroscopic level by arranging the cavities.


Acta Physica Sinica. 2006 55(3): 1153-1159. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1153-1159. article doi:10.7498/aps.55.1153 10.7498/aps.55.1153 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1153 1153-1159
<![CDATA[Influence of energy-transfer up-conversion on upper level lifetime of Tm, Ho:YLF Q-switched laser]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1160

Based the energy transfer between energy levels and the transition between ions of diode-end-pumped Tm,Ho:YLF laser, with consideration of energy transfer up-conversion, the rate equations of Tm,Ho:YLF Q-switched laser are given, and the analytical formulas of single pulse energy is deduced from the rate-equations. It is shown theoretically that the energy transfer up-conversion reduces not only the single pulse energy but also the upper level lifetime of Tm,Ho:YLF Q-switched laser. An experiment is carefully designed to verify these conclusions.


Acta Physica Sinica. 2006 55(3): 1160-1164. Published 2006-03-20 ]]>

Based the energy transfer between energy levels and the transition between ions of diode-end-pumped Tm,Ho:YLF laser, with consideration of energy transfer up-conversion, the rate equations of Tm,Ho:YLF Q-switched laser are given, and the analytical formulas of single pulse energy is deduced from the rate-equations. It is shown theoretically that the energy transfer up-conversion reduces not only the single pulse energy but also the upper level lifetime of Tm,Ho:YLF Q-switched laser. An experiment is carefully designed to verify these conclusions.


Acta Physica Sinica. 2006 55(3): 1160-1164. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1160-1164. article doi:10.7498/aps.55.1160 10.7498/aps.55.1160 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1160 1160-1164
<![CDATA[Multifrequency dynamical model of pulsed CO2 lasers]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1165

A six-temperature multifrequency dynamical model of pulsed CO2 lasers is presented, taking account of the collision-dependent overlap of rotational lines, the effect of hot bands and sequence bands on the gain spectrum, and non-Lorentzian line overlap effect in a wide range of pressures from 20 torr to 20 atm. Theoretical calculations of pulse shape and laser spectrum have good agreement with experimental results. This model should be useful in the understanding of pulsed CO2 laser dynamics, in the evaluation of alternative pump schemes, and in the investigation of tunable characteristics. Thus it can provide theoretical support for the design of pulsed CO2 lasers.


Acta Physica Sinica. 2006 55(3): 1165-1170. Published 2006-03-20 ]]>

A six-temperature multifrequency dynamical model of pulsed CO2 lasers is presented, taking account of the collision-dependent overlap of rotational lines, the effect of hot bands and sequence bands on the gain spectrum, and non-Lorentzian line overlap effect in a wide range of pressures from 20 torr to 20 atm. Theoretical calculations of pulse shape and laser spectrum have good agreement with experimental results. This model should be useful in the understanding of pulsed CO2 laser dynamics, in the evaluation of alternative pump schemes, and in the investigation of tunable characteristics. Thus it can provide theoretical support for the design of pulsed CO2 lasers.


Acta Physica Sinica. 2006 55(3): 1165-1170. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1165-1170. article doi:10.7498/aps.55.1165 10.7498/aps.55.1165 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1165 1165-1170
<![CDATA[High average power Q-switched quasi-continue-wave Nd:YAG laser]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1171

A high-average-power and high-beam-quality diode-side-pumped solid-state Q-switched laser was developed by use of low concentration Nd:YAG crystals with thermally near-unstable resonator design and two-rod birefringence compensation technology. Two orthogonal acousto-optic Q-switches were used to sustain fully holding of the pump gain. The 1064 nm quasi-continuous-wave average output power of 258 W at pump power of 1116 W was achieved with the beam quality factor M2~15.5 at a repetition rate of 10 kHz and a pulse width of 64 ns, corresponding to a peek power of 0.4GW and an optical-to-optical conversion efficiency of 23.1%.


Acta Physica Sinica. 2006 55(3): 1171-1175. Published 2006-03-20 ]]>

A high-average-power and high-beam-quality diode-side-pumped solid-state Q-switched laser was developed by use of low concentration Nd:YAG crystals with thermally near-unstable resonator design and two-rod birefringence compensation technology. Two orthogonal acousto-optic Q-switches were used to sustain fully holding of the pump gain. The 1064 nm quasi-continuous-wave average output power of 258 W at pump power of 1116 W was achieved with the beam quality factor M2~15.5 at a repetition rate of 10 kHz and a pulse width of 64 ns, corresponding to a peek power of 0.4GW and an optical-to-optical conversion efficiency of 23.1%.


Acta Physica Sinica. 2006 55(3): 1171-1175. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1171-1175. article doi:10.7498/aps.55.1171 10.7498/aps.55.1171 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1171 1171-1175
<![CDATA[Three dimensional pondermotive scattering of ultrashort electron beam in the field of focused ultraintense laser pulse]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1176

Using a three-dimensional test particle simulation code, we study the pondermotive scattering of an ultrashort electron beam subject to a focused ultraintense femtosecond laser pulse. The dependence of the spatial distribution of electron beam and electron energy spectrum on the time delay between laser pulse and electron pulse is discussed in detail. Through the measurement of the spatial distribution of electron beam or electron spectrum, we present a method to measure the duration of an ultrashort electron pulse.


Acta Physica Sinica. 2006 55(3): 1176-1180. Published 2006-03-20 ]]>

Using a three-dimensional test particle simulation code, we study the pondermotive scattering of an ultrashort electron beam subject to a focused ultraintense femtosecond laser pulse. The dependence of the spatial distribution of electron beam and electron energy spectrum on the time delay between laser pulse and electron pulse is discussed in detail. Through the measurement of the spatial distribution of electron beam or electron spectrum, we present a method to measure the duration of an ultrashort electron pulse.


Acta Physica Sinica. 2006 55(3): 1176-1180. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1176-1180. article doi:10.7498/aps.55.1176 10.7498/aps.55.1176 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1176 1176-1180
<![CDATA[Modeling RAL experiment to test our simulation]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1181

A code series for transient collisional excitation (TCE ) was newly developed based on the previous code series for QSS scheme, the TCE Ne-like Ge 19.6nm X-ray laser experiment done by RAL in 2000 was modeled to test our code series, a relatively good fit is obtained which provides convenience for our study of TCE scheme.


Acta Physica Sinica. 2006 55(3): 1181-1185. Published 2006-03-20 ]]>

A code series for transient collisional excitation (TCE ) was newly developed based on the previous code series for QSS scheme, the TCE Ne-like Ge 19.6nm X-ray laser experiment done by RAL in 2000 was modeled to test our code series, a relatively good fit is obtained which provides convenience for our study of TCE scheme.


Acta Physica Sinica. 2006 55(3): 1181-1185. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1181-1185. article doi:10.7498/aps.55.1181 10.7498/aps.55.1181 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1181 1181-1185
<![CDATA[Doppler-free three-photon resonant six-wave mixing]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1186

We study the three-photon resonant six-wave mixing (SWM) with phase-conjugation geometry in Doppler system. The theoretical calculation indicates that the signal spectrum is Doppler-free when the laser line width is narrow. This technique provides a new spectroscopic tool for studying the highly excited atomic or molecular states with high resolution. It has advantages of uncritical phase matching condition, excellent spatial signal resolution and simple optical alignment.


Acta Physica Sinica. 2006 55(3): 1186-1190. Published 2006-03-20 ]]>

We study the three-photon resonant six-wave mixing (SWM) with phase-conjugation geometry in Doppler system. The theoretical calculation indicates that the signal spectrum is Doppler-free when the laser line width is narrow. This technique provides a new spectroscopic tool for studying the highly excited atomic or molecular states with high resolution. It has advantages of uncritical phase matching condition, excellent spatial signal resolution and simple optical alignment.


Acta Physica Sinica. 2006 55(3): 1186-1190. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1186-1190. article doi:10.7498/aps.55.1186 10.7498/aps.55.1186 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1186 1186-1190
<![CDATA[Ultrashort pulse Yb3+-doped fiber ring laser with all-fiber structure]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1191

Theory of the self-starting passive mode-locked Yb3+-doped fiber ring laser generating short pulses is presented. The ultrashort pulse Yb3+-doped fiber ring laser with all-fiber structure has been designed and turned out. Two 976nm LD pumped lasers are used as the pump sources and high concentration Yb3+-doped fiber is adopted as gain medium. Using the nonlinear polarization rotation (NPR) effect of the fiber, self-starting stable mode-locked pulse is obtained. The mode-locked threshold power of the laser is 260mW and the output power is 25mW. The center wavelength of the mode-locked pulse is 1056nm with 3dB bandwidth of 11.7nm at repetition rate of 20MHz. Comparing with the other structures of the fiber lasers, the structure we adopted is more efficient and has better stability.


Acta Physica Sinica. 2006 55(3): 1191-1195. Published 2006-03-20 ]]>

Theory of the self-starting passive mode-locked Yb3+-doped fiber ring laser generating short pulses is presented. The ultrashort pulse Yb3+-doped fiber ring laser with all-fiber structure has been designed and turned out. Two 976nm LD pumped lasers are used as the pump sources and high concentration Yb3+-doped fiber is adopted as gain medium. Using the nonlinear polarization rotation (NPR) effect of the fiber, self-starting stable mode-locked pulse is obtained. The mode-locked threshold power of the laser is 260mW and the output power is 25mW. The center wavelength of the mode-locked pulse is 1056nm with 3dB bandwidth of 11.7nm at repetition rate of 20MHz. Comparing with the other structures of the fiber lasers, the structure we adopted is more efficient and has better stability.


Acta Physica Sinica. 2006 55(3): 1191-1195. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1191-1195. article doi:10.7498/aps.55.1191 10.7498/aps.55.1191 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1191 1191-1195
<![CDATA[Output characteristics of LD end-pumped Nd:YVO4 solid-state laser with flat-flat cavity]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1196

Internal factors (thermal lens,cavity lengths,enabled aperture etc) restricting the output of the LD end-pumped Nd:YVO4 solid-state laser with flat-flat cavity is studied. A reasonable explaination is given and a way of improving the output is pointed out through the graphic analysis of the transmitting and transforming circle.


Acta Physica Sinica. 2006 55(3): 1196-1200. Published 2006-03-20 ]]>

Internal factors (thermal lens,cavity lengths,enabled aperture etc) restricting the output of the LD end-pumped Nd:YVO4 solid-state laser with flat-flat cavity is studied. A reasonable explaination is given and a way of improving the output is pointed out through the graphic analysis of the transmitting and transforming circle.


Acta Physica Sinica. 2006 55(3): 1196-1200. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1196-1200. article doi:10.7498/aps.55.1196 10.7498/aps.55.1196 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1196 1196-1200
<![CDATA[Experimental research of laser-induced damage mechanism of the sol-gel SiO2 and IBSD SiO2 thin films]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1201

This paper investigates the high-power laser-induced damage of two types of single-layer SiO2 thin films on K9 substrate, which are respectively deposited by IBSD technique and sol-gel technique, and have the same substrate parameters and the same film thickness. They were tested by surface thermal lensing technique to obtain the thermal absorbance and the dynamic response. The results show that the laser-initiated damage threshold of Sol-Gel SiO2 thin film is far higher than that of IBSD SiO2 thin film. And combined with threshold measurement and the microscopic observation, this paper well explains in detail the threshold difference between Sol-Gel SiO2 and IBSD SiO2 thin films.


Acta Physica Sinica. 2006 55(3): 1201-1206. Published 2006-03-20 ]]>

This paper investigates the high-power laser-induced damage of two types of single-layer SiO2 thin films on K9 substrate, which are respectively deposited by IBSD technique and sol-gel technique, and have the same substrate parameters and the same film thickness. They were tested by surface thermal lensing technique to obtain the thermal absorbance and the dynamic response. The results show that the laser-initiated damage threshold of Sol-Gel SiO2 thin film is far higher than that of IBSD SiO2 thin film. And combined with threshold measurement and the microscopic observation, this paper well explains in detail the threshold difference between Sol-Gel SiO2 and IBSD SiO2 thin films.


Acta Physica Sinica. 2006 55(3): 1201-1206. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1201-1206. article doi:10.7498/aps.55.1201 10.7498/aps.55.1201 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1201 1201-1206
<![CDATA[Spectroscopic characteristics of transparent Yb:Y2-2xLa2xO3 laser ceramics]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1207

It was first reported the spectral properties of a low-temperature sintered transparent Yb:Y2-2xLa2xO3 laser ceramics. Yb:Y2-2xLa2xO3 laser ceramics have broad absorption band and large absorption cross-section of 4.0×10-20cm2 at wavelengths 977nm of the highest absorption peak. Its fluorescence lifetime is 1.1ms, and the emission cross-sections are 1.0×10-20cm2 and 0.7×10-20cm2 at wavelengths 1033nm and 1077nm, respectively. All the optical properties are similar to those of single crystals.


Acta Physica Sinica. 2006 55(3): 1207-1210. Published 2006-03-20 ]]>

It was first reported the spectral properties of a low-temperature sintered transparent Yb:Y2-2xLa2xO3 laser ceramics. Yb:Y2-2xLa2xO3 laser ceramics have broad absorption band and large absorption cross-section of 4.0×10-20cm2 at wavelengths 977nm of the highest absorption peak. Its fluorescence lifetime is 1.1ms, and the emission cross-sections are 1.0×10-20cm2 and 0.7×10-20cm2 at wavelengths 1033nm and 1077nm, respectively. All the optical properties are similar to those of single crystals.


Acta Physica Sinica. 2006 55(3): 1207-1210. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1207-1210. article doi:10.7498/aps.55.1207 10.7498/aps.55.1207 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1207 1207-1210
<![CDATA[Study on Z-scan characteristics for large optical nonlinear phase shift]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1211

Using Gaussian decomposition (GD) method, we studied the theory of Z-scan with large nonlinear phase shift induced by a pulsed laser. It has been verified that the GD method is still valid to deal with analysis of Z-scan measurements with large nonlinear phase shift. By comparing the peak-valley configuration of the Z-scan curves for large nonlinear phase shift induced by pulsed and CW laser, we found that some new peak-valley features of the Z-scan curves appear as the aperture size or light intensity increases in the case of large nonlinear phase shift. Meanwhile, we carried out the Z-scan experiments of pure CS2 to confirm the results of numerical simulation in the case of large nonlinear phase shift induced by a picosecond pulsed laser. The experimental results agree well with the theoretical. Our results have some significance to the measurement of Z-scan with large nonlinear phase shift induced by a pulsed laser.


Acta Physica Sinica. 2006 55(3): 1211-1217. Published 2006-03-20 ]]>

Using Gaussian decomposition (GD) method, we studied the theory of Z-scan with large nonlinear phase shift induced by a pulsed laser. It has been verified that the GD method is still valid to deal with analysis of Z-scan measurements with large nonlinear phase shift. By comparing the peak-valley configuration of the Z-scan curves for large nonlinear phase shift induced by pulsed and CW laser, we found that some new peak-valley features of the Z-scan curves appear as the aperture size or light intensity increases in the case of large nonlinear phase shift. Meanwhile, we carried out the Z-scan experiments of pure CS2 to confirm the results of numerical simulation in the case of large nonlinear phase shift induced by a picosecond pulsed laser. The experimental results agree well with the theoretical. Our results have some significance to the measurement of Z-scan with large nonlinear phase shift induced by a pulsed laser.


Acta Physica Sinica. 2006 55(3): 1211-1217. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1211-1217. article doi:10.7498/aps.55.1211 10.7498/aps.55.1211 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1211 1211-1217
<![CDATA[Coherence enhancement of spatially incoherent light beams through soliton interaction in logarithmically saturable nonlinear media]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1218

We investigate numerically the interaction between incoherent spatial solitons in a nonlinear medium with logarithmic saturable nonlinearity base on the coherent density approach. Numerical simulations show that both the intensity and the spatial coherence can be greatly enhanced through soliton interaction. At the same time, we show that the soliton interaction can be controlled by the total partial incoherence, which can not only suppress the coherent soliton interaction such as attractive, repulsive or exchange energy, but also induce weak attractive due to incoherent superposition of two incoherent solitons.


Acta Physica Sinica. 2006 55(3): 1218-1223. Published 2006-03-20 ]]>

We investigate numerically the interaction between incoherent spatial solitons in a nonlinear medium with logarithmic saturable nonlinearity base on the coherent density approach. Numerical simulations show that both the intensity and the spatial coherence can be greatly enhanced through soliton interaction. At the same time, we show that the soliton interaction can be controlled by the total partial incoherence, which can not only suppress the coherent soliton interaction such as attractive, repulsive or exchange energy, but also induce weak attractive due to incoherent superposition of two incoherent solitons.


Acta Physica Sinica. 2006 55(3): 1218-1223. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1218-1223. article doi:10.7498/aps.55.1218 10.7498/aps.55.1218 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1218 1218-1223
<![CDATA[Stimulated Brillouin scattering reflection pumped by broadband KrF laser]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1224

Stimulated Brillouin scattering (SBS) reflectivity as a function of pump power density, pressure of medium and focal length for broadband KrF laser pump was investigated experimentally. SBS reflectivity increases nonlinearly, approaches to saturation and decreases with the pump power density increasing. The pressure in the medium makes the SBS reflectivity to increase. SBS saturation has a peak value with the focal length from 10cm to 100cm. Broadband multimode SBS model has been built theoretically. Experimental results agree well with the model.


Acta Physica Sinica. 2006 55(3): 1224-1230. Published 2006-03-20 ]]>

Stimulated Brillouin scattering (SBS) reflectivity as a function of pump power density, pressure of medium and focal length for broadband KrF laser pump was investigated experimentally. SBS reflectivity increases nonlinearly, approaches to saturation and decreases with the pump power density increasing. The pressure in the medium makes the SBS reflectivity to increase. SBS saturation has a peak value with the focal length from 10cm to 100cm. Broadband multimode SBS model has been built theoretically. Experimental results agree well with the model.


Acta Physica Sinica. 2006 55(3): 1224-1230. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1224-1230. article doi:10.7498/aps.55.1224 10.7498/aps.55.1224 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1224 1224-1230
<![CDATA[Pump source angle tuning in quasi-phase matched optical parametric oscillator]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1231

This paper systemically presents a theoretical analysis on pump source angle tuning in quasi-phase matched (QPM) optical parametric oscillator (OPO) in periodically poled crystal. The precise formula and the formula in paraxial approximation, both of which describe the relationship between rotation angle of pump source and wavelengths of pump, signal and idler wave in QPM OPO, are presented. It is found that the idler wave and the pump wave for signal-resonated OPO propagate along the same side of the crystal x-axis to exit, as propagate the signal wave and the pump wave for idler-resonated OPO. In addition, the separation angle between the signal wave and the idler wave for signal-resonated OPO is greater than that for idler-resonated OPO. More importantly, the tuning rate for signal-resonated OPO is also greater than that for idler-resonated OPO.


Acta Physica Sinica. 2006 55(3): 1231-1236. Published 2006-03-20 ]]>

This paper systemically presents a theoretical analysis on pump source angle tuning in quasi-phase matched (QPM) optical parametric oscillator (OPO) in periodically poled crystal. The precise formula and the formula in paraxial approximation, both of which describe the relationship between rotation angle of pump source and wavelengths of pump, signal and idler wave in QPM OPO, are presented. It is found that the idler wave and the pump wave for signal-resonated OPO propagate along the same side of the crystal x-axis to exit, as propagate the signal wave and the pump wave for idler-resonated OPO. In addition, the separation angle between the signal wave and the idler wave for signal-resonated OPO is greater than that for idler-resonated OPO. More importantly, the tuning rate for signal-resonated OPO is also greater than that for idler-resonated OPO.


Acta Physica Sinica. 2006 55(3): 1231-1236. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1231-1236. article doi:10.7498/aps.55.1231 10.7498/aps.55.1231 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1231 1231-1236
<![CDATA[Strongly nonlocal elliptical spatial optical soliton]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1237

We investigate the propagation of the elliptical Gussian beam in strongly nonlocal nonlinear media with an elliptically symmetric response.We derive analytical formulas for the evolution of the beam parameters and conditions for the formation of nonlocal elliptical spatial optical soliton.


Acta Physica Sinica. 2006 55(3): 1237-1243. Published 2006-03-20 ]]>

We investigate the propagation of the elliptical Gussian beam in strongly nonlocal nonlinear media with an elliptically symmetric response.We derive analytical formulas for the evolution of the beam parameters and conditions for the formation of nonlocal elliptical spatial optical soliton.


Acta Physica Sinica. 2006 55(3): 1237-1243. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1237-1243. article doi:10.7498/aps.55.1237 10.7498/aps.55.1237 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1237 1237-1243
<![CDATA[Analysis of band gap in honeycomb photonic crystal heterostructure]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1244

In the present paper, a new kind of honeycomb photonic crystal heterostructure(PCH) is proposed. The band gap structure of this photonic crystal heterostructure is investigated with supercell technique based on the plane-wave expansion method. The configuration of heterostructure and the corresponding band structures are obtained and the guide modes are analyzed. Furthermore, the influences of longitudinal sideslipping and transverse displacement of lattices on the band gap structures are discussed. It may provide a new configuration to generate guide modes. The achieved results show that the guide modes can exist in this heterostructure without any shift of lattices, and guide modes are highly sensitive to transverse shift, while sideslipping affects guide modes only slightly.


Acta Physica Sinica. 2006 55(3): 1244-1247. Published 2006-03-20 ]]>

In the present paper, a new kind of honeycomb photonic crystal heterostructure(PCH) is proposed. The band gap structure of this photonic crystal heterostructure is investigated with supercell technique based on the plane-wave expansion method. The configuration of heterostructure and the corresponding band structures are obtained and the guide modes are analyzed. Furthermore, the influences of longitudinal sideslipping and transverse displacement of lattices on the band gap structures are discussed. It may provide a new configuration to generate guide modes. The achieved results show that the guide modes can exist in this heterostructure without any shift of lattices, and guide modes are highly sensitive to transverse shift, while sideslipping affects guide modes only slightly.


Acta Physica Sinica. 2006 55(3): 1244-1247. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1244-1247. article doi:10.7498/aps.55.1244 10.7498/aps.55.1244 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1244 1244-1247
<![CDATA[Optical properties of semiconductor quantum-well material using photonic crystal fabricated by micro-fabrication machine]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1248

Two-dimensional photonic crystals in near infrared region were fabricated by using the focused ion beam (FIB) method and the method of electron-beam lithography (EBL) combined with dry etching. Both methods can fabricate perfect crystals, the method of FIB is simple,the other is more complicated. It is shown that the material with the photonic crystal fabricated by FIB has no fluorescence,on the other hand, the small-lattice photonic crystal made by EBL combined with dry etching can enhance the extraction efficiency two folds, though the photonic crystal has some disorder. The mechanisms of the enhanced-emission and the absence of emission are also discussed.


Acta Physica Sinica. 2006 55(3): 1248-1252. Published 2006-03-20 ]]>

Two-dimensional photonic crystals in near infrared region were fabricated by using the focused ion beam (FIB) method and the method of electron-beam lithography (EBL) combined with dry etching. Both methods can fabricate perfect crystals, the method of FIB is simple,the other is more complicated. It is shown that the material with the photonic crystal fabricated by FIB has no fluorescence,on the other hand, the small-lattice photonic crystal made by EBL combined with dry etching can enhance the extraction efficiency two folds, though the photonic crystal has some disorder. The mechanisms of the enhanced-emission and the absence of emission are also discussed.


Acta Physica Sinica. 2006 55(3): 1248-1252. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1248-1252. article doi:10.7498/aps.55.1248 10.7498/aps.55.1248 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1248 1248-1252
<![CDATA[Study of 3D optical chain with highly focused vector beam]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1253

We present a design of diffractive optical element to produce 3D optical chain along optical axis near the focus of a high numerical aperture (NA) lens by spatially modulating the phase of incoming vector beam. This optical chain can trap multiple individual particles in three dimensions at different planes near the focus. For flexibly controlling this special optical trapping system, we systematically analize the factors affecting the characteristics of the optical chain, such as different incoming vector polarization of light, the NA of the lens, and the structure of the DOE.


Acta Physica Sinica. 2006 55(3): 1253-1258. Published 2006-03-20 ]]>

We present a design of diffractive optical element to produce 3D optical chain along optical axis near the focus of a high numerical aperture (NA) lens by spatially modulating the phase of incoming vector beam. This optical chain can trap multiple individual particles in three dimensions at different planes near the focus. For flexibly controlling this special optical trapping system, we systematically analize the factors affecting the characteristics of the optical chain, such as different incoming vector polarization of light, the NA of the lens, and the structure of the DOE.


Acta Physica Sinica. 2006 55(3): 1253-1258. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1253-1258. article doi:10.7498/aps.55.1253 10.7498/aps.55.1253 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1253 1253-1258
<![CDATA[Electroabsorption-modulated laser light-source module using selective area growth for 10 Gb/s transmission]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1259

In this work, a novel light source of strained InGaAsP/InGaAsP MQW EAM monolithically integrated with DFB laser is fabricated by ultra-low-pressure (22×102Pa) selective area growth (SAG) MOCVD technique. Superior device performances have been obtained, such as low threshold current of 19 mA, output light power of about 7 mW, and over 16 dB extinction ratio at 5 V applied voltage when coupled into a single mode fiber. Over 10 GHz 3 dB bandwidth in EAM part is developed with a driving voltage of 3 V. After the chip is packaged into a 7-pin butterfly compact module, 10-Gb/s NRZ transmission experiments are successfully performed in standard fiber. A clearly-open eye diagram is achieved in the module output with over 8.3 dB dynamic extinction ratio. Power penalty less than 1.5 dB has been obtained after transmission through 53.3 km of standard fiber, which demonstrates that high-speed, low chirp EAM/DFB integrated light source can be obtained by ultra-low-pressure (22×10\+2Pa) SAG method.


Acta Physica Sinica. 2006 55(3): 1259-1263. Published 2006-03-20 ]]>

In this work, a novel light source of strained InGaAsP/InGaAsP MQW EAM monolithically integrated with DFB laser is fabricated by ultra-low-pressure (22×102Pa) selective area growth (SAG) MOCVD technique. Superior device performances have been obtained, such as low threshold current of 19 mA, output light power of about 7 mW, and over 16 dB extinction ratio at 5 V applied voltage when coupled into a single mode fiber. Over 10 GHz 3 dB bandwidth in EAM part is developed with a driving voltage of 3 V. After the chip is packaged into a 7-pin butterfly compact module, 10-Gb/s NRZ transmission experiments are successfully performed in standard fiber. A clearly-open eye diagram is achieved in the module output with over 8.3 dB dynamic extinction ratio. Power penalty less than 1.5 dB has been obtained after transmission through 53.3 km of standard fiber, which demonstrates that high-speed, low chirp EAM/DFB integrated light source can be obtained by ultra-low-pressure (22×10\+2Pa) SAG method.


Acta Physica Sinica. 2006 55(3): 1259-1263. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1259-1263. article doi:10.7498/aps.55.1259 10.7498/aps.55.1259 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1259 1259-1263
<![CDATA[Investigation on holographic algorithm and experiment of combined wave superposition approach]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1264

The general nerar-field acoustic holography (NAH) cannot reconstruct the surface acoustic information of each coherent acoustic source in coherent acoustic field,which has more than one acoustic sources with the same frequency, and they cannot realize holographic reconstruction and prediction of the independent acoustic field generated by one coherent acoustic source too.So the holographic reconstruction and prediction of coherent acoustic field has become the foremost problem to be resolved in the application of NAH. On the basis of the proposed combined wave superposition approach, an experiment is carried out to realize the holographic reconstruction and prediction of a coherent acoustic filed generated by two sound boxes.By this experiment,the feasibility and accuracy of combined wave superposition approach are demonstrated,the shortcoming of general wave superposition approach in holographic construction and prediction of coherent acoustic field are also demonstrated.The Tikhonov regularization method is proposed to control the ill-posedness of inverse acoustic problem, and the principle of filter coefficient selection is also studied.The experiment indicates that Tikhonov regularization method with appropriate filter coefficient can improve the precision of the holographic reconstruction and prediction.


Acta Physica Sinica. 2006 55(3): 1264-1270. Published 2006-03-20 ]]>

The general nerar-field acoustic holography (NAH) cannot reconstruct the surface acoustic information of each coherent acoustic source in coherent acoustic field,which has more than one acoustic sources with the same frequency, and they cannot realize holographic reconstruction and prediction of the independent acoustic field generated by one coherent acoustic source too.So the holographic reconstruction and prediction of coherent acoustic field has become the foremost problem to be resolved in the application of NAH. On the basis of the proposed combined wave superposition approach, an experiment is carried out to realize the holographic reconstruction and prediction of a coherent acoustic filed generated by two sound boxes.By this experiment,the feasibility and accuracy of combined wave superposition approach are demonstrated,the shortcoming of general wave superposition approach in holographic construction and prediction of coherent acoustic field are also demonstrated.The Tikhonov regularization method is proposed to control the ill-posedness of inverse acoustic problem, and the principle of filter coefficient selection is also studied.The experiment indicates that Tikhonov regularization method with appropriate filter coefficient can improve the precision of the holographic reconstruction and prediction.


Acta Physica Sinica. 2006 55(3): 1264-1270. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1264-1270. article doi:10.7498/aps.55.1264 10.7498/aps.55.1264 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1264 1264-1270
<![CDATA[Temperature distribution of microstructure fiber preform during fiber drawing]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1271

Drawing temperature is an important factor affecting the structure of microstructure fibers (MSF) during MSF drawing. According to the Fourier equation of time-dependent heat conduction with, original conditions and boundary conditions of MSF preform, the temperature distribution equation of MSF preform is derived in cylindrical coordinates. It is shown the feeding speed of MSF preform is optimal when the temperature distribution of MSF preform is close to the steady-state heat conduction in high temperature furnace, then the temperature of high temperature furnace can be lowered to the intenerate temperature of MSF preform. In addition, the optimal speed will be increased if the air-filling fraction of MSF preform is high.


Acta Physica Sinica. 2006 55(3): 1271-1275. Published 2006-03-20 ]]>

Drawing temperature is an important factor affecting the structure of microstructure fibers (MSF) during MSF drawing. According to the Fourier equation of time-dependent heat conduction with, original conditions and boundary conditions of MSF preform, the temperature distribution equation of MSF preform is derived in cylindrical coordinates. It is shown the feeding speed of MSF preform is optimal when the temperature distribution of MSF preform is close to the steady-state heat conduction in high temperature furnace, then the temperature of high temperature furnace can be lowered to the intenerate temperature of MSF preform. In addition, the optimal speed will be increased if the air-filling fraction of MSF preform is high.


Acta Physica Sinica. 2006 55(3): 1271-1275. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1271-1275. article doi:10.7498/aps.55.1271 10.7498/aps.55.1271 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1271 1271-1275
<![CDATA[Information preservation method for micro-scale flow with temperature variation]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1276

Based on the information preservation(IP) method, a simple effective temperature model is presented. The IP method with new temperature model can simulate the flow which has temperature variation. Moreover, studies show that when the local density gradient of the simulated flow is large, it will cause numerical divergence if the second order central difference scheme of the mass conservation equation is used to update the information density. So the first order upwind scheme is recommended to update the information density for the flow with large density gradient.


Acta Physica Sinica. 2006 55(3): 1276-1282. Published 2006-03-20 ]]>

Based on the information preservation(IP) method, a simple effective temperature model is presented. The IP method with new temperature model can simulate the flow which has temperature variation. Moreover, studies show that when the local density gradient of the simulated flow is large, it will cause numerical divergence if the second order central difference scheme of the mass conservation equation is used to update the information density. So the first order upwind scheme is recommended to update the information density for the flow with large density gradient.


Acta Physica Sinica. 2006 55(3): 1276-1282. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1276-1282. article doi:10.7498/aps.55.1276 10.7498/aps.55.1276 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1276 1276-1282
<![CDATA[FDTD simulation for magnetized plasma photonic crystals]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1283

Magnetized plasma photonic crystals are artificial periodic structures composed of magnetized plasmas and dielectric structures (or vacuum).In this paper,the piecewise linear current density recursive convolution (PLCDRC) finite-difference time-domain (FDTD) method for magnetized plasmas is applied to study the magnetized plasma photonic crystals.The effect of parameters of magnetized plasma on electromagnetic band gap is presented.In time-domain,the electromagnetic propagation process and reflection/transmission electric field of Gaussian pulses through magnetized plasma photonic crystals are investigated.In frequency-domain,the reflection and transmission coefficients through magnetized plasma photonic crystals are computed.The results are discussed.


Acta Physica Sinica. 2006 55(3): 1283-1288. Published 2006-03-20 ]]>

Magnetized plasma photonic crystals are artificial periodic structures composed of magnetized plasmas and dielectric structures (or vacuum).In this paper,the piecewise linear current density recursive convolution (PLCDRC) finite-difference time-domain (FDTD) method for magnetized plasmas is applied to study the magnetized plasma photonic crystals.The effect of parameters of magnetized plasma on electromagnetic band gap is presented.In time-domain,the electromagnetic propagation process and reflection/transmission electric field of Gaussian pulses through magnetized plasma photonic crystals are investigated.In frequency-domain,the reflection and transmission coefficients through magnetized plasma photonic crystals are computed.The results are discussed.


Acta Physica Sinica. 2006 55(3): 1283-1288. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1283-1288. article doi:10.7498/aps.55.1283 10.7498/aps.55.1283 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1283 1283-1288
<![CDATA[Study of soft X-ray energy spectra from gas-puff Z-pinch plasma]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1289

A ROSS-FILTER-PIN spectrometer in the spectral range of 0.28keV —1.56keV was developed to study the soft X-ray radiation emitted from gas-puff Z-pinch plasma. It is composed of five channels covering the energy interval of interest without gaps. Soft X-ray spectral energy cuts were determined by the L absorption edges of selected filter elements (K absorption edges being used for light filter elements), and the optimum thickness of filter material was designed using computer code. To minimize the residual sensitivity outside the sensitivity range of each channel, element of the first filter was added into the second filter of all the Ross pair. To diminish the area of each filter, PIN detector with small sensitive area of 1 mm2 was adopted for the spectrometer. A filter with small area is easy to fabricate and would be helpful to withstand the Z-pinch discharge shock wave. With this ROSS-FILTER-PIN spectrometer, the energy spectra of soft X-ray from a small gas-puff Z-pinch were investigated, and the correlation between the soft X-ray yield and the plasma implosion state was also studied.


Acta Physica Sinica. 2006 55(3): 1289-1294. Published 2006-03-20 ]]>

A ROSS-FILTER-PIN spectrometer in the spectral range of 0.28keV —1.56keV was developed to study the soft X-ray radiation emitted from gas-puff Z-pinch plasma. It is composed of five channels covering the energy interval of interest without gaps. Soft X-ray spectral energy cuts were determined by the L absorption edges of selected filter elements (K absorption edges being used for light filter elements), and the optimum thickness of filter material was designed using computer code. To minimize the residual sensitivity outside the sensitivity range of each channel, element of the first filter was added into the second filter of all the Ross pair. To diminish the area of each filter, PIN detector with small sensitive area of 1 mm2 was adopted for the spectrometer. A filter with small area is easy to fabricate and would be helpful to withstand the Z-pinch discharge shock wave. With this ROSS-FILTER-PIN spectrometer, the energy spectra of soft X-ray from a small gas-puff Z-pinch were investigated, and the correlation between the soft X-ray yield and the plasma implosion state was also studied.


Acta Physica Sinica. 2006 55(3): 1289-1294. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1289-1294. article doi:10.7498/aps.55.1289 10.7498/aps.55.1289 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1289 1289-1294
<![CDATA[Electromagnetic performance of plane delamination media with ITO transparent conductive film]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1295

Electromagnetic performances of multilayer plane delamination media with an ITO (indium tin oxide) transparent conductive film have been researched theoretically and the calculated curve well agrees with the measured curve.The research shows that the electromagnetic performances of the multilayer media are related to ITO (with sheet resistance 8Ω) film's interface location,the layer number of the plane delamination media and the thickness of the plane delamination media,and so on.An optimized system of four-layer plane delamination mediums with a thickness of only 7.35mm and very large electromagnetic reflectance within the rauge of 8—18GHz has been designed.The sheet resistance of the ITO film in the multilayer plane delamination media should be less than 30Ω,and the smaller the sheet resistance,the langer the electromagnetic reflectance of the multilayer plane delamination media.


Acta Physica Sinica. 2006 55(3): 1295-1300. Published 2006-03-20 ]]>

Electromagnetic performances of multilayer plane delamination media with an ITO (indium tin oxide) transparent conductive film have been researched theoretically and the calculated curve well agrees with the measured curve.The research shows that the electromagnetic performances of the multilayer media are related to ITO (with sheet resistance 8Ω) film's interface location,the layer number of the plane delamination media and the thickness of the plane delamination media,and so on.An optimized system of four-layer plane delamination mediums with a thickness of only 7.35mm and very large electromagnetic reflectance within the rauge of 8—18GHz has been designed.The sheet resistance of the ITO film in the multilayer plane delamination media should be less than 30Ω,and the smaller the sheet resistance,the langer the electromagnetic reflectance of the multilayer plane delamination media.


Acta Physica Sinica. 2006 55(3): 1295-1300. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1295-1300. article doi:10.7498/aps.55.1295 10.7498/aps.55.1295 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1295 1295-1300
<![CDATA[Simulation on heating of plasma in a magnetic field with electrostatic wave]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1301

A uniform nonlinear resonant condition for interaction between electrostatic wave and charged particles in a uniform magnetic field is given by multi-scale expansion.It is verified by numerical simulation.It is shown that resonant heating can be produced by electrostatic wave with sub-harmonic frequency of the cyclotron.Moreover,it is shown that the heating efficiency does not increase with the amplitude of driving wave even if for the same frequency,which means there is an optimum combination of frequency and amplitude to get efficient heating.


Acta Physica Sinica. 2006 55(3): 1301-1306. Published 2006-03-20 ]]>

A uniform nonlinear resonant condition for interaction between electrostatic wave and charged particles in a uniform magnetic field is given by multi-scale expansion.It is verified by numerical simulation.It is shown that resonant heating can be produced by electrostatic wave with sub-harmonic frequency of the cyclotron.Moreover,it is shown that the heating efficiency does not increase with the amplitude of driving wave even if for the same frequency,which means there is an optimum combination of frequency and amplitude to get efficient heating.


Acta Physica Sinica. 2006 55(3): 1301-1306. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1301-1306. article doi:10.7498/aps.55.1301 10.7498/aps.55.1301 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1301 1301-1306
<![CDATA[Electron cyclotron current drive under different operational regimes in tokamak plasma]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1307

With a given density profile of plasma,the temperature profiles of the plasma operating in the negative central magnetic shear mode,the H-mode and L-mode of conventional magnetic shear,are calculated respectively by applying the energy equation of electrons and ions,according to the thermal conductivity in different operational regimes.And then the electron cyclotron current drive and wave power deposition in the above modes are investigated with the relativistic Fokker-Planck equation incorporated into a ray tracing code.The result shows that in the mode of negative central magnetic shear,the current drive efficiency is the highest,meanwhile the zones of power deposition and current profile are wide.In the H-mode of conventional magnetic shear,the current drive efficiency is low,and the zones of power deposition and current profile are narrow.In the L-mode of conventional magnetic shear,the current drive efficiency is the lowest,the zones of power deposition and current profile are very narrow.


Acta Physica Sinica. 2006 55(3): 1307-1314. Published 2006-03-20 ]]>

With a given density profile of plasma,the temperature profiles of the plasma operating in the negative central magnetic shear mode,the H-mode and L-mode of conventional magnetic shear,are calculated respectively by applying the energy equation of electrons and ions,according to the thermal conductivity in different operational regimes.And then the electron cyclotron current drive and wave power deposition in the above modes are investigated with the relativistic Fokker-Planck equation incorporated into a ray tracing code.The result shows that in the mode of negative central magnetic shear,the current drive efficiency is the highest,meanwhile the zones of power deposition and current profile are wide.In the H-mode of conventional magnetic shear,the current drive efficiency is low,and the zones of power deposition and current profile are narrow.In the L-mode of conventional magnetic shear,the current drive efficiency is the lowest,the zones of power deposition and current profile are very narrow.


Acta Physica Sinica. 2006 55(3): 1307-1314. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1307-1314. article doi:10.7498/aps.55.1307 10.7498/aps.55.1307 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1307 1307-1314
<![CDATA[Real-time determination of plasma confinement parameters in HL-2A]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1315

During the plasma discharge in HL-2A, the magnetic field at the plasma boundary is computed using currents filaments code. The Shafranov integrals S1,S2 and S3 are deduced; the poloidal beta, internal inductance, the horizontal position of the magnetic axis Rm and the plasma energy Wdia are calculated; the current center of plasma (Rc,Zc)is computed with the current moments. The real time determination of these quantities is of significance for understanding and adjusting the HL-2A discharge in time, and for improving plasma performance.


Acta Physica Sinica. 2006 55(3): 1315-1319. Published 2006-03-20 ]]>

During the plasma discharge in HL-2A, the magnetic field at the plasma boundary is computed using currents filaments code. The Shafranov integrals S1,S2 and S3 are deduced; the poloidal beta, internal inductance, the horizontal position of the magnetic axis Rm and the plasma energy Wdia are calculated; the current center of plasma (Rc,Zc)is computed with the current moments. The real time determination of these quantities is of significance for understanding and adjusting the HL-2A discharge in time, and for improving plasma performance.


Acta Physica Sinica. 2006 55(3): 1315-1319. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1315-1319. article doi:10.7498/aps.55.1315 10.7498/aps.55.1315 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1315 1315-1319
<![CDATA[Molecular dynamics simulation of the correlation between the viscosity and structure of liquid metal]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1320

The non-equilibrium molecular dynamics simulation (NEMD) has been performed based on the embeded atom potential to obtain the pair correlation function and the viscosity of liquid Al.The pair correlation function by the simulation agrees well with Waseda's X\|ray diffraction measurement.The temperature dependence of viscosity meets the Arrhenius formula:η=Aexp(E/RT) and the activation energy E calculated is 15968.27J/mol.The expression between the viscosity, pair correlation function and the inter-atomic potential has been obtained by application of the simulated viscosity value and the activation energy to meet L-J potential.The two fitted curves of viscosity agree well with that obtained by the NEMD method,showing the fitting program we compiled is excellent and the fitting to the L-J potential is achieved.This present work provides a new method to explore inter-atomic potential.


Acta Physica Sinica. 2006 55(3): 1320-1324. Published 2006-03-20 ]]>

The non-equilibrium molecular dynamics simulation (NEMD) has been performed based on the embeded atom potential to obtain the pair correlation function and the viscosity of liquid Al.The pair correlation function by the simulation agrees well with Waseda's X\|ray diffraction measurement.The temperature dependence of viscosity meets the Arrhenius formula:η=Aexp(E/RT) and the activation energy E calculated is 15968.27J/mol.The expression between the viscosity, pair correlation function and the inter-atomic potential has been obtained by application of the simulated viscosity value and the activation energy to meet L-J potential.The two fitted curves of viscosity agree well with that obtained by the NEMD method,showing the fitting program we compiled is excellent and the fitting to the L-J potential is achieved.This present work provides a new method to explore inter-atomic potential.


Acta Physica Sinica. 2006 55(3): 1320-1324. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1320-1324. article doi:10.7498/aps.55.1320 10.7498/aps.55.1320 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1320 1320-1324
<![CDATA[New computing methods and programs for separating multipe-broadening effects of X-ray diffraction lines]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1325

The least square method and corresponding computing programs for separating twofold broadening effects due to the crystallite-microstress, crystallite-stacking faults, microstress-stacking faults and three-fold effect of crystallite-stress-faults have been proposed and established. The least square method can be applied to closed packing hexagonal (cph), face-centered cubic (fcc) and body-centered cubic (bcc) structures. A few examples are presented and discussed.


Acta Physica Sinica. 2006 55(3): 1325-1335. Published 2006-03-20 ]]>

The least square method and corresponding computing programs for separating twofold broadening effects due to the crystallite-microstress, crystallite-stacking faults, microstress-stacking faults and three-fold effect of crystallite-stress-faults have been proposed and established. The least square method can be applied to closed packing hexagonal (cph), face-centered cubic (fcc) and body-centered cubic (bcc) structures. A few examples are presented and discussed.


Acta Physica Sinica. 2006 55(3): 1325-1335. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1325-1335. article doi:10.7498/aps.55.1325 10.7498/aps.55.1325 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1325 1325-1335
<![CDATA[The sine-squared potential and properties of planar channelling radiation of positron]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1336

The sine-squared potential is introduce to describe the interaction between particles and the crystal.The motion equation of the planar channelling particles is reduced to the pendulum equatione by this interaction potential.The solution of the equation and the period of the particle motion are expressed exactly by means of Jacobian elliptic function and elliptic integral.The radiation intensity and properties of the radiation spectrum are discussed.It is point out that it is possible to take channeling radiation as a new γ-Laser.


Acta Physica Sinica. 2006 55(3): 1336-1340. Published 2006-03-20 ]]>

The sine-squared potential is introduce to describe the interaction between particles and the crystal.The motion equation of the planar channelling particles is reduced to the pendulum equatione by this interaction potential.The solution of the equation and the period of the particle motion are expressed exactly by means of Jacobian elliptic function and elliptic integral.The radiation intensity and properties of the radiation spectrum are discussed.It is point out that it is possible to take channeling radiation as a new γ-Laser.


Acta Physica Sinica. 2006 55(3): 1336-1340. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1336-1340. article doi:10.7498/aps.55.1336 10.7498/aps.55.1336 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1336 1336-1340
<![CDATA[Simulation of dendritic growth of multicomponent alloys using phase-field method]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1341

A phase-field model for multicomponent alloys based on the binary phase-field model has been developed. The isothermal dendritic growth of Al-Si-Mg alloys is presented as a numerical example, accordingly, the dendrite growing morphology of multicomponent alloys solidification could be simulated realistically using the phase-field model. As the result, the intricate figures such as secondary and tertiary dendrite arms are revealed. The decrease of solute Mg can trigger the growth of the secondary arms and increase the solute microsegregation rate, the tip speed and radius of dendrite. The variation of the speed and the radius in the dendrite tip agrees well with theoretical and experimental results in succinonitrile-acetone system. In addition, the spines of the primary arms have lowest concentration, and the mushy regions between the dendrite secondary arms have the highest concentration; the solute gradients are higher in the vicinity of the S/L interface regions, and highest in the tip.


Acta Physica Sinica. 2006 55(3): 1341-1345. Published 2006-03-20 ]]>

A phase-field model for multicomponent alloys based on the binary phase-field model has been developed. The isothermal dendritic growth of Al-Si-Mg alloys is presented as a numerical example, accordingly, the dendrite growing morphology of multicomponent alloys solidification could be simulated realistically using the phase-field model. As the result, the intricate figures such as secondary and tertiary dendrite arms are revealed. The decrease of solute Mg can trigger the growth of the secondary arms and increase the solute microsegregation rate, the tip speed and radius of dendrite. The variation of the speed and the radius in the dendrite tip agrees well with theoretical and experimental results in succinonitrile-acetone system. In addition, the spines of the primary arms have lowest concentration, and the mushy regions between the dendrite secondary arms have the highest concentration; the solute gradients are higher in the vicinity of the S/L interface regions, and highest in the tip.


Acta Physica Sinica. 2006 55(3): 1341-1345. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1341-1345. article doi:10.7498/aps.55.1341 10.7498/aps.55.1341 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1341 1341-1345
<![CDATA[Comparison of temperature-dependent dielectric characteristic in two different (Ba,Sr)TiO3 films]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1346

A high dielectric constant of 2500 near room temperature was observed in (Ba0.5Sr0.5)TiO3 (BSTO) film prepared by pulsed-laser deposition (PLD) on Pt/Ti/SiO2/Si (100) substrate at 550℃ in N2 atmosphere. The dielectric constant is weakly temperature dependent above 200 K. The dielectric behavior of this film is different from the BSTO film deposited in the O2 atmosphere, but very similar to that reported for the so-called “colossal” dielectric constant materials, such as CaCu3Ti4O12. The film prepared in O2 atmosphere at 650℃ shows normal ferroelectric phase transition, which are fitted with Curie-Weiss law. However, for the film prepared in N2 atmosphere at 550℃, the temperature dependence of dielectric relaxation can be characterized by a thermally excited relaxation process. Such anomalous dielectric response of the BST films is ascribed to the formation of the Schottky barrier between the metallic electrode and the film surface.


Acta Physica Sinica. 2006 55(3): 1346-1350. Published 2006-03-20 ]]>

A high dielectric constant of 2500 near room temperature was observed in (Ba0.5Sr0.5)TiO3 (BSTO) film prepared by pulsed-laser deposition (PLD) on Pt/Ti/SiO2/Si (100) substrate at 550℃ in N2 atmosphere. The dielectric constant is weakly temperature dependent above 200 K. The dielectric behavior of this film is different from the BSTO film deposited in the O2 atmosphere, but very similar to that reported for the so-called “colossal” dielectric constant materials, such as CaCu3Ti4O12. The film prepared in O2 atmosphere at 650℃ shows normal ferroelectric phase transition, which are fitted with Curie-Weiss law. However, for the film prepared in N2 atmosphere at 550℃, the temperature dependence of dielectric relaxation can be characterized by a thermally excited relaxation process. Such anomalous dielectric response of the BST films is ascribed to the formation of the Schottky barrier between the metallic electrode and the film surface.


Acta Physica Sinica. 2006 55(3): 1346-1350. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1346-1350. article doi:10.7498/aps.55.1346 10.7498/aps.55.1346 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1346 1346-1350
<![CDATA[Study of low energy sputtering of Pt(111) surface by molecular dynamics simulation]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1351

Low energy sputtering of Pt (111) surface by noble metal atoms with the incident energy in the range of 0.1 — 200 eV has been studied by molecular dynamics sim ulation. The atomic interaction potential with embedded atom method (EAM) was us ed in the simulation. It was found that the sputtering threshold energy is indep endent of the mass of the incident atom in the case of normal impact on the Pt ( 111) surface. When the incident energy is lower than the threshold energy, the b ehavior of incident atom can be regarded as deposition process. When the inciden t energy is higher than the threshold energy, however, the sputtering yield incr eases with the increase of the incident energy. For the incident energy of 200 e V, the sputtering yield induced by various incident atoms approaches 1 or even h igher. The results mean that the atom with incident energy higher than 200 eV ma inly plays the role of sputtering. The probability of angular distribution of th e sputtered atoms and the sputtering pattern are similar to the sputtering resul ts with higher incident energy. We found that the sputtering yield is a function of the reduced energy of incident atom and the mass ratio of incident atom to t arget atom when the incident energy is higher than the threshold energy, which i s different from the linear cascade theory based on the binary collision model. We suggest a new physical mechanism for low energy sputtering, where the reflect ion of incident atom by target atom dominates the sputtering process of surface atoms.


Acta Physica Sinica. 2006 55(3): 1351-1357. Published 2006-03-20 ]]>

Low energy sputtering of Pt (111) surface by noble metal atoms with the incident energy in the range of 0.1 — 200 eV has been studied by molecular dynamics sim ulation. The atomic interaction potential with embedded atom method (EAM) was us ed in the simulation. It was found that the sputtering threshold energy is indep endent of the mass of the incident atom in the case of normal impact on the Pt ( 111) surface. When the incident energy is lower than the threshold energy, the b ehavior of incident atom can be regarded as deposition process. When the inciden t energy is higher than the threshold energy, however, the sputtering yield incr eases with the increase of the incident energy. For the incident energy of 200 e V, the sputtering yield induced by various incident atoms approaches 1 or even h igher. The results mean that the atom with incident energy higher than 200 eV ma inly plays the role of sputtering. The probability of angular distribution of th e sputtered atoms and the sputtering pattern are similar to the sputtering resul ts with higher incident energy. We found that the sputtering yield is a function of the reduced energy of incident atom and the mass ratio of incident atom to t arget atom when the incident energy is higher than the threshold energy, which i s different from the linear cascade theory based on the binary collision model. We suggest a new physical mechanism for low energy sputtering, where the reflect ion of incident atom by target atom dominates the sputtering process of surface atoms.


Acta Physica Sinica. 2006 55(3): 1351-1357. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1351-1357. article doi:10.7498/aps.55.1351 10.7498/aps.55.1351 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1351 1351-1357
<![CDATA[Nucleation-growth and spinodal decomposition of zinc oxide films prepared by sol-gel technique]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1358

Transparent zinc oxide (ZnO) films were prepared on ZnWO4 crystal by sol-gel technique. Surface morphology of ZnO films were observed with optical mi croscope. The results of show that ZnO films are formed in three different stage s from nucleation on surface, grain growth to island formation. Because ZnO crys tal nucleus were grown under non_equilibrium condition, it is inevitable that de ndrite growth, fractal growth and spinodal decomposition phenomenon are involved in the growing process.


Acta Physica Sinica. 2006 55(3): 1358-1362. Published 2006-03-20 ]]>

Transparent zinc oxide (ZnO) films were prepared on ZnWO4 crystal by sol-gel technique. Surface morphology of ZnO films were observed with optical mi croscope. The results of show that ZnO films are formed in three different stage s from nucleation on surface, grain growth to island formation. Because ZnO crys tal nucleus were grown under non_equilibrium condition, it is inevitable that de ndrite growth, fractal growth and spinodal decomposition phenomenon are involved in the growing process.


Acta Physica Sinica. 2006 55(3): 1358-1362. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1358-1362. article doi:10.7498/aps.55.1358 10.7498/aps.55.1358 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1358 1358-1362
<![CDATA[Characterization of silicon nitride films prepared by MW-ECR magnetron sputtering]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1363

Hydrogen-free silicon nitride films were deposited at room temperature by microw ave electron cyclotron resonance (ECR) plasma source enhanced unbalanced magnetr on sputtering system. Fourier-transform infrared spectroscopy and X-ray photoele ctron spectroscopy were used to study the bond type, the change of bond structur es, and the stoichiometry of the silicon nitride films. Atomic-force microscopy and nano-indentation were used to study the morphological features and mechanica l characteristics of the films. The results indicate that the structure and char acteristics of the films deposited by this technique depend strongly on the dens ity of sputtered Si in plasma and the films deposited at 4 sccm N2 fl ow show excellent stoichiometry and properties.


Acta Physica Sinica. 2006 55(3): 1363-1368. Published 2006-03-20 ]]>

Hydrogen-free silicon nitride films were deposited at room temperature by microw ave electron cyclotron resonance (ECR) plasma source enhanced unbalanced magnetr on sputtering system. Fourier-transform infrared spectroscopy and X-ray photoele ctron spectroscopy were used to study the bond type, the change of bond structur es, and the stoichiometry of the silicon nitride films. Atomic-force microscopy and nano-indentation were used to study the morphological features and mechanica l characteristics of the films. The results indicate that the structure and char acteristics of the films deposited by this technique depend strongly on the dens ity of sputtered Si in plasma and the films deposited at 4 sccm N2 fl ow show excellent stoichiometry and properties.


Acta Physica Sinica. 2006 55(3): 1363-1368. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1363-1368. article doi:10.7498/aps.55.1363 10.7498/aps.55.1363 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1363 1363-1368
<![CDATA[The grain boundary segregation of microalloying elements and the ultra-refinement of steel]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1369

A model of Σ5〈001〉/(210) high angle grain boundary (GB) in austenite phase in steel was set up with computer programming. The environment-sensitive embedding energies (ESE) of C, N and microalloying elements in grains or in GB core are c alculated by recursion method, respectively. The segregation and interaction of C, N and microalloying elements in the GB core were discussed. Calculation resul ts show that: discrete light impurities C and N tend to segregate in the GB area , forming atomic clusters; microalloying elements are liable to distribute in pe rfect austenite grains. Ti, V, Nb occupy the top sites of the trigonal prism for med by iron in the GB core, and Ti, V, Nb can also form atomic clusters in GB co re like C or N. When the temperature is decreased and the concentration of C, N and microalloying elements reach to the limit of solubility, the C, N compounds of microalloying elements precipitate from the matrix in GB core of austenite in steel. These compounds can act as heterogeneous nuclei of austenite phase in th e course of recrystallization and retard the growth of austenite grains, leading to the refinement of austenite grains. Nb is the most efficient refiner of micr oalloying elements Nb, Ti, V.


Acta Physica Sinica. 2006 55(3): 1369-1373. Published 2006-03-20 ]]>

A model of Σ5〈001〉/(210) high angle grain boundary (GB) in austenite phase in steel was set up with computer programming. The environment-sensitive embedding energies (ESE) of C, N and microalloying elements in grains or in GB core are c alculated by recursion method, respectively. The segregation and interaction of C, N and microalloying elements in the GB core were discussed. Calculation resul ts show that: discrete light impurities C and N tend to segregate in the GB area , forming atomic clusters; microalloying elements are liable to distribute in pe rfect austenite grains. Ti, V, Nb occupy the top sites of the trigonal prism for med by iron in the GB core, and Ti, V, Nb can also form atomic clusters in GB co re like C or N. When the temperature is decreased and the concentration of C, N and microalloying elements reach to the limit of solubility, the C, N compounds of microalloying elements precipitate from the matrix in GB core of austenite in steel. These compounds can act as heterogeneous nuclei of austenite phase in th e course of recrystallization and retard the growth of austenite grains, leading to the refinement of austenite grains. Nb is the most efficient refiner of micr oalloying elements Nb, Ti, V.


Acta Physica Sinica. 2006 55(3): 1369-1373. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1369-1373. article doi:10.7498/aps.55.1369 10.7498/aps.55.1369 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1369 1369-1373
<![CDATA[Geometries and the electronic structures of t-HfO2 (001) surface]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1374

The geometries and the electronic structures of t-HfO2 and its (001) surface have been studied by first-principle calculations using the density func tional theory (DFT). The optimized results show that the t-HfO2 (001) surface has no surface reconstruction. Compared with the bulk electronic struct ure, the density of states (DOS) of t-HfO2 (001) surface is higher th an that of the bulk. In addition, the DOS of t-HfO2 (001) surface is closer to the Fermi level. The valence band has the tendency to move toward the lower energy, resulting in the formation of a new surface state. The band gap of t-HfO2 (001) surface is much smaller than that of bulk band gap. The existence of a new surface state and the reduction of band gap are due to the r eduction of the Hf and O surface coordination which are different from the bulk atoms.


Acta Physica Sinica. 2006 55(3): 1374-1378. Published 2006-03-20 ]]>

The geometries and the electronic structures of t-HfO2 and its (001) surface have been studied by first-principle calculations using the density func tional theory (DFT). The optimized results show that the t-HfO2 (001) surface has no surface reconstruction. Compared with the bulk electronic struct ure, the density of states (DOS) of t-HfO2 (001) surface is higher th an that of the bulk. In addition, the DOS of t-HfO2 (001) surface is closer to the Fermi level. The valence band has the tendency to move toward the lower energy, resulting in the formation of a new surface state. The band gap of t-HfO2 (001) surface is much smaller than that of bulk band gap. The existence of a new surface state and the reduction of band gap are due to the r eduction of the Hf and O surface coordination which are different from the bulk atoms.


Acta Physica Sinica. 2006 55(3): 1374-1378. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1374-1378. article doi:10.7498/aps.55.1374 10.7498/aps.55.1374 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1374 1374-1378
<![CDATA[Study of persistent photoconductivity and subband electronic properties of the two-dimensional electron gas in modulation doped GaAs/AlGaAs structure]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1379

We obtained the high mobility of μ2K=1.78×106 cm2/V·s in Si-doped GaAs/AlGaAs two-dimensional electron gas (2DEG) structures . After the sample was illuminated by a light-emitting diode in magnetic fields up to 6 T at T=2K, we did observe the persistent photoconductivity effect and th e electron density increased obviously. The electronic properties of 2DEG have b een studied by Quantum-Hall-effect and Shubnikov-de Haas (SdH) oscillation measu rements. We found that the electron concentrations of two subbands increase simu ltaneity with the increasing total electron concentration, and the electron mobi lity also increases obviously after being illuminated. At the same time, we also found that the electronic quantum lifetime becomes shorter, and a theoretical e xplunation is given through the widths of integral quantum Hall plateaus.


Acta Physica Sinica. 2006 55(3): 1379-1383. Published 2006-03-20 ]]>

We obtained the high mobility of μ2K=1.78×106 cm2/V·s in Si-doped GaAs/AlGaAs two-dimensional electron gas (2DEG) structures . After the sample was illuminated by a light-emitting diode in magnetic fields up to 6 T at T=2K, we did observe the persistent photoconductivity effect and th e electron density increased obviously. The electronic properties of 2DEG have b een studied by Quantum-Hall-effect and Shubnikov-de Haas (SdH) oscillation measu rements. We found that the electron concentrations of two subbands increase simu ltaneity with the increasing total electron concentration, and the electron mobi lity also increases obviously after being illuminated. At the same time, we also found that the electronic quantum lifetime becomes shorter, and a theoretical e xplunation is given through the widths of integral quantum Hall plateaus.


Acta Physica Sinica. 2006 55(3): 1379-1383. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1379-1383. article doi:10.7498/aps.55.1379 10.7498/aps.55.1379 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1379 1379-1383
<![CDATA[Noise as a representation for reliability of light emitting diode]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1384

Through the research of the internal structure of Light Emitting Diode (LED), we discovered that the interface trap density and diffusion current ratio are key factors determining the performance of LED, and they are also closely related to the reliability of LED. Among the many kinds of internal noises in LED, low-fre quency 1/f noise describes the interfoce trap density and diffuse current ratio effectively. Based on the mechanism of carrier number fluctuation and carrier mo bility fluctuation of 1/f noise, we put forward the electrical model and 1/f noi se model of LED. We also measured the electrical noise of the device over a wide range of current. Experimental results agree well with the proposed model. Usin g the experimental data, the relationship between noise and the performance and reliability of LED is established. It is proved that the larger the noise magnit ude, the nearer the current exponent is to 2, leading to the degradation of devi ce reliability and significant rise in device invalidation rate.


Acta Physica Sinica. 2006 55(3): 1384-1389. Published 2006-03-20 ]]>

Through the research of the internal structure of Light Emitting Diode (LED), we discovered that the interface trap density and diffusion current ratio are key factors determining the performance of LED, and they are also closely related to the reliability of LED. Among the many kinds of internal noises in LED, low-fre quency 1/f noise describes the interfoce trap density and diffuse current ratio effectively. Based on the mechanism of carrier number fluctuation and carrier mo bility fluctuation of 1/f noise, we put forward the electrical model and 1/f noi se model of LED. We also measured the electrical noise of the device over a wide range of current. Experimental results agree well with the proposed model. Usin g the experimental data, the relationship between noise and the performance and reliability of LED is established. It is proved that the larger the noise magnit ude, the nearer the current exponent is to 2, leading to the degradation of devi ce reliability and significant rise in device invalidation rate.


Acta Physica Sinica. 2006 55(3): 1384-1389. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1384-1389. article doi:10.7498/aps.55.1384 10.7498/aps.55.1384 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1384 1384-1389
<![CDATA[Influences of growth temperature on the crystalline characteristics and optical properties for ZnO films deposited by reactive magnetron sputtering]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1390

Using reactive radio-frequency magnetron sputtering, ZnO films with strong c-axi s orientation have been deposited on Si (100) substrates at temperatures ranging from room temperature (RT) to 750℃. We have studied the influence of growth te mperature on the structural characteristics of the as-deposited films in morphol ogy, grain size, microstructure, and residual stress by using atomic force micro scopy, transmission electron microscopy, X-ray diffraction, and Raman spectrosco py. With the measurement of the transmission spectra and photoluminescence (PL) properties, the relationship between the crystallinity and optical properties of ZnO films have been discussed. It is found that the grain size increases with t emperature up to 500℃, and then decreases at 750℃. ZnO grains have an epitaxia l relationship with Si (100) substrate for the films deposited at the temperatur es ranging from RT to 750℃. The films deposited below 500℃ are in the states o f compressive strain while the film deposited at 750℃ is in tensile. The differ ence in growth temperature results in the variation of refractive index, extinct ion coefficient, optical energy gap, and PL properties of the films. It is concl uded that growth temperature dominates the PL behavior of ZnO films. We also dis cuss the physical mechanism affecting the PL behavior.


Acta Physica Sinica. 2006 55(3): 1390-1397. Published 2006-03-20 ]]>

Using reactive radio-frequency magnetron sputtering, ZnO films with strong c-axi s orientation have been deposited on Si (100) substrates at temperatures ranging from room temperature (RT) to 750℃. We have studied the influence of growth te mperature on the structural characteristics of the as-deposited films in morphol ogy, grain size, microstructure, and residual stress by using atomic force micro scopy, transmission electron microscopy, X-ray diffraction, and Raman spectrosco py. With the measurement of the transmission spectra and photoluminescence (PL) properties, the relationship between the crystallinity and optical properties of ZnO films have been discussed. It is found that the grain size increases with t emperature up to 500℃, and then decreases at 750℃. ZnO grains have an epitaxia l relationship with Si (100) substrate for the films deposited at the temperatur es ranging from RT to 750℃. The films deposited below 500℃ are in the states o f compressive strain while the film deposited at 750℃ is in tensile. The differ ence in growth temperature results in the variation of refractive index, extinct ion coefficient, optical energy gap, and PL properties of the films. It is concl uded that growth temperature dominates the PL behavior of ZnO films. We also dis cuss the physical mechanism affecting the PL behavior.


Acta Physica Sinica. 2006 55(3): 1390-1397. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1390-1397. article doi:10.7498/aps.55.1390 10.7498/aps.55.1390 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1390 1390-1397
<![CDATA[Growth of ZnO microrod array films and their optical properties]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1398

A novel approach using low-cost and simple-equipment was successfully demonstrat ed on the growth of ZnO microrod array films. Scanning electron microscopy (SEM) and X-ray diffraction (XRD) has characterized the microstructure of the samples . The results indicate that ZnO microrod array films are hexagonal, highly orien ted crystalline array films, grown along c-axis of ZnO on (0001) sapphire substr ates. The FWHM is about 1.8° for the (0004) rocking curve of the ZnO films. The photoluminescence spectra of ZnO array films show a strong and narrow peak at 395nm.


Acta Physica Sinica. 2006 55(3): 1398-1401. Published 2006-03-20 ]]>

A novel approach using low-cost and simple-equipment was successfully demonstrat ed on the growth of ZnO microrod array films. Scanning electron microscopy (SEM) and X-ray diffraction (XRD) has characterized the microstructure of the samples . The results indicate that ZnO microrod array films are hexagonal, highly orien ted crystalline array films, grown along c-axis of ZnO on (0001) sapphire substr ates. The FWHM is about 1.8° for the (0004) rocking curve of the ZnO films. The photoluminescence spectra of ZnO array films show a strong and narrow peak at 395nm.


Acta Physica Sinica. 2006 55(3): 1398-1401. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1398-1401. article doi:10.7498/aps.55.1398 10.7498/aps.55.1398 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1398 1398-1401
<![CDATA[The effects of passivation and temperature on the barrier strain of Al0.22Ga0.78N/GaN heterostructures]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1402

The barrier strain in Al0.22Ga0.78N/GaN heterostructure, w ith and without Si3N4 passivation layer, was investigated at temperatures from room temperature to 813K by using high resolution X-ray dif fraction. The strain relaxation occurs when the temperature exceeds 523K for the unpassivated Al0.22Ga0.78N layers. After passivation, an initial increase of the strain with increasing temperature is observed in Al0.22Ga0.78N layers, and at the higher temperatures the strain only decreases slightly in the 100-nm-thick Al0.22Ga0.78N layer, but a pronounced strain relaxation occurs in the 50-nm-thick one due to the fact that the thickness of the A10.22Ga0.78N layer is close to the critical thickness, and hence the increase of tensile strain induce d by passivation will result in partial strain relaxation via the formation of c racks or the gliding motion and multiplication of dislocations.


Acta Physica Sinica. 2006 55(3): 1402-1406. Published 2006-03-20 ]]>

The barrier strain in Al0.22Ga0.78N/GaN heterostructure, w ith and without Si3N4 passivation layer, was investigated at temperatures from room temperature to 813K by using high resolution X-ray dif fraction. The strain relaxation occurs when the temperature exceeds 523K for the unpassivated Al0.22Ga0.78N layers. After passivation, an initial increase of the strain with increasing temperature is observed in Al0.22Ga0.78N layers, and at the higher temperatures the strain only decreases slightly in the 100-nm-thick Al0.22Ga0.78N layer, but a pronounced strain relaxation occurs in the 50-nm-thick one due to the fact that the thickness of the A10.22Ga0.78N layer is close to the critical thickness, and hence the increase of tensile strain induce d by passivation will result in partial strain relaxation via the formation of c racks or the gliding motion and multiplication of dislocations.


Acta Physica Sinica. 2006 55(3): 1402-1406. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1402-1406. article doi:10.7498/aps.55.1402 10.7498/aps.55.1402 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1402 1402-1406
<![CDATA[Deep level transient spectroscopy studies of Er and Pr implanted GaN films]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1407

Deep level transient spectroscopy measurements were used to characterize the ele ctrical properties of metal organic chemical vapor deposition grown undoped, Er- implanted and Pr-implanted GaN films. Only one deep level located at 0.270 eV be low the conduction band was found in the as-grown GaN films. But four defect le vels located at 0.300 eV, 0.188 eV, 0.600 eV and 0.410 eV below the conduction b and were found in the Er-implanted GaN films after annealing at 900 ℃ for 30 mi n, and four defect levels located at 0.280 eV, 0.190 eV, 0.610 eV and 0.390 eV b elow the conduction band were found in the Pr-implanted GaN films after annealin g at 1050 ℃ for 30min. The origins of the deep defect levels are discussed. Aft er annealing at 900℃ for 30min in a nitrogen flow, Er-related 1538nm luminescen ce peaks could be observed for the Er-implanted GaN sample. The energy-transfer and luminescence mechanism of the Er-implanted GaN film are described.


Acta Physica Sinica. 2006 55(3): 1407-1412. Published 2006-03-20 ]]>

Deep level transient spectroscopy measurements were used to characterize the ele ctrical properties of metal organic chemical vapor deposition grown undoped, Er- implanted and Pr-implanted GaN films. Only one deep level located at 0.270 eV be low the conduction band was found in the as-grown GaN films. But four defect le vels located at 0.300 eV, 0.188 eV, 0.600 eV and 0.410 eV below the conduction b and were found in the Er-implanted GaN films after annealing at 900 ℃ for 30 mi n, and four defect levels located at 0.280 eV, 0.190 eV, 0.610 eV and 0.390 eV b elow the conduction band were found in the Pr-implanted GaN films after annealin g at 1050 ℃ for 30min. The origins of the deep defect levels are discussed. Aft er annealing at 900℃ for 30min in a nitrogen flow, Er-related 1538nm luminescen ce peaks could be observed for the Er-implanted GaN sample. The energy-transfer and luminescence mechanism of the Er-implanted GaN film are described.


Acta Physica Sinica. 2006 55(3): 1407-1412. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1407-1412. article doi:10.7498/aps.55.1407 10.7498/aps.55.1407 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1407 1407-1412
<![CDATA[Kondo effect in parallel double quantum dots embedded in a mesoscopic ring]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1413

We theoretically studied the properties of the ground state of the parallel-coup led double quantum dot embedded in a mesoscopic ring in the Kondo regime by mean s of the two-impurity Anderson Hamiltonian. The Hamiltonian is solved by means o f the slave-boson mean-field theory. Our results show that when the system goes into the strong coupling regime, two parallel dots can be coupled coherently, wh ich leads to an enhanced Kondo effect and a giant persistent current emerging in this system. This double quantum dot device can be a candidate for future devic e applications.


Acta Physica Sinica. 2006 55(3): 1413-1418. Published 2006-03-20 ]]>

We theoretically studied the properties of the ground state of the parallel-coup led double quantum dot embedded in a mesoscopic ring in the Kondo regime by mean s of the two-impurity Anderson Hamiltonian. The Hamiltonian is solved by means o f the slave-boson mean-field theory. Our results show that when the system goes into the strong coupling regime, two parallel dots can be coupled coherently, wh ich leads to an enhanced Kondo effect and a giant persistent current emerging in this system. This double quantum dot device can be a candidate for future devic e applications.


Acta Physica Sinica. 2006 55(3): 1413-1418. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1413-1418. article doi:10.7498/aps.55.1413 10.7498/aps.55.1413 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1413 1413-1418
<![CDATA[Negative bias temperature instability of HfN/HfO2 gated p-MOSFETs]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1419

The negative-bias temperature instability (NBTI) characteristics of HfN/HfO 2 gated p-MOSFET with equivalent oxide thickness (EOT) of 1.3nm and low pre-existi ng traps are studied. Due to the low pre-existing trap density of HfN/HfO2 ga te stack, the observed NBTI characteristics are intrinsic, rather induced by the fabricating process. The observed characteristics can be compared with those re ported in SiO2 based gate stack and can be explained with the general ized reac tion-diffusion (R-D) model: under negative bias and temperature stressing, holes injected from the Si substrate could cause the Si-H bond breaking at the Si sub strate interface. The H atoms diffuse away into the bulk layer and the Si+ spe cies are left at the interface. The diffusing H atoms and the left Si+ species cause the NBTI characteristics.


Acta Physica Sinica. 2006 55(3): 1419-1423. Published 2006-03-20 ]]>

The negative-bias temperature instability (NBTI) characteristics of HfN/HfO 2 gated p-MOSFET with equivalent oxide thickness (EOT) of 1.3nm and low pre-existi ng traps are studied. Due to the low pre-existing trap density of HfN/HfO2 ga te stack, the observed NBTI characteristics are intrinsic, rather induced by the fabricating process. The observed characteristics can be compared with those re ported in SiO2 based gate stack and can be explained with the general ized reac tion-diffusion (R-D) model: under negative bias and temperature stressing, holes injected from the Si substrate could cause the Si-H bond breaking at the Si sub strate interface. The H atoms diffuse away into the bulk layer and the Si+ spe cies are left at the interface. The diffusing H atoms and the left Si+ species cause the NBTI characteristics.


Acta Physica Sinica. 2006 55(3): 1419-1423. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1419-1423. article doi:10.7498/aps.55.1419 10.7498/aps.55.1419 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1419 1419-1423
<![CDATA[Growth of p-GaN at low temperature and its properties as light emitting diodes]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1424

The p-type GaN(p-GaN) samples grown at low temperature 870—980℃ on sapphire su bstrate were prepared by the metal organic chemical vapor deposition technique(M OCVD), and their electrical properties were investigated. The p-GaN samples grow n below 900℃ show high-resistivity, and samples grown at above 900℃ have good conductivity. In addition, the electrical properties are also related with the d oping level and the growth condition of p-GaN. The low N-Ga mole ratio leads to poor conductivity, the high ratio leads to rough morphology. At last, we use the optimized p-GaN to fabricate the green-light emitting diodes.We found that when the growth temperature is lower, the luminescence intensity and reverse voltage is higher but the forward voltage increases slightly.


Acta Physica Sinica. 2006 55(3): 1424-1429. Published 2006-03-20 ]]>

The p-type GaN(p-GaN) samples grown at low temperature 870—980℃ on sapphire su bstrate were prepared by the metal organic chemical vapor deposition technique(M OCVD), and their electrical properties were investigated. The p-GaN samples grow n below 900℃ show high-resistivity, and samples grown at above 900℃ have good conductivity. In addition, the electrical properties are also related with the d oping level and the growth condition of p-GaN. The low N-Ga mole ratio leads to poor conductivity, the high ratio leads to rough morphology. At last, we use the optimized p-GaN to fabricate the green-light emitting diodes.We found that when the growth temperature is lower, the luminescence intensity and reverse voltage is higher but the forward voltage increases slightly.


Acta Physica Sinica. 2006 55(3): 1424-1429. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1424-1429. article doi:10.7498/aps.55.1424 10.7498/aps.55.1424 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1424 1424-1429
<![CDATA[Study of the transport properties of self-assembled alkanethiol monolayer by conduction atomic force microscopy]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1430

Self-assembled alkanethiol monolayers (SAMs) were prepared on the Au(111) substr ate. The behavior of the transport properties of SAMs under external load was in vestigated by the conduction atomic force microscopy. The current of SAM was fou nd to increase with the external load, and this property can be well characteriz ed by the Hertz model. It was also found that the conductance of SAM decreases e xponentially with the chain length of the alkanethiol molecules. The correspondi ng current decay constant β is demonstrated to decrease with the external load at first, and then becomes independent of the external load. Furthermore, the cu rrent of SAM with long chain molecules increases more apparently than that with short ones. These features all originate from the tunneling effect via nearby mo lecular chains for the charges.


Acta Physica Sinica. 2006 55(3): 1430-1434. Published 2006-03-20 ]]>

Self-assembled alkanethiol monolayers (SAMs) were prepared on the Au(111) substr ate. The behavior of the transport properties of SAMs under external load was in vestigated by the conduction atomic force microscopy. The current of SAM was fou nd to increase with the external load, and this property can be well characteriz ed by the Hertz model. It was also found that the conductance of SAM decreases e xponentially with the chain length of the alkanethiol molecules. The correspondi ng current decay constant β is demonstrated to decrease with the external load at first, and then becomes independent of the external load. Furthermore, the cu rrent of SAM with long chain molecules increases more apparently than that with short ones. These features all originate from the tunneling effect via nearby mo lecular chains for the charges.


Acta Physica Sinica. 2006 55(3): 1430-1434. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1430-1434. article doi:10.7498/aps.55.1430 10.7498/aps.55.1430 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1430 1430-1434
<![CDATA[Influence of the stress on the transport behavior of La0.83Sr0.17MnO3 film]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1435

The LSMO (x=0.17) film on the Si (111) substrate was fabricated by the sol-gel m ethod.The R-T curves, the infrared spectra and XRD results of the block and the film with different thickness show that the crystals of the LSMO films are orth ogonal, and the film orientation has some relation with the film thickness. Whe n the film thickness lies between the 450nm to 680 nm, the orientation is 〈200 〉, but when the film thickness equals to 900 nm, the orientation is 〈020〉. Ac cording to the reactive energy and the harmonic oscillator model, the relational expressions, between the infrared absorption and the Mn-O-Mn bond length and bo nd angel were studied. The infrared absorption near 600cm-1 relates t o the different lattice constant b, and the metal-insulator transformation tempe ratures (TMI) of the block material and the films differ much, those of the films being much lower than that of the block material and, at the same time, has something to do with the film thickness. The paper indicates that the stress in the LSMO films inducing the lattice constant change and then arousing the change of bond angel and JT effect is the main reason for the change of the transformation temperature.


Acta Physica Sinica. 2006 55(3): 1435-1440. Published 2006-03-20 ]]>

The LSMO (x=0.17) film on the Si (111) substrate was fabricated by the sol-gel m ethod.The R-T curves, the infrared spectra and XRD results of the block and the film with different thickness show that the crystals of the LSMO films are orth ogonal, and the film orientation has some relation with the film thickness. Whe n the film thickness lies between the 450nm to 680 nm, the orientation is 〈200 〉, but when the film thickness equals to 900 nm, the orientation is 〈020〉. Ac cording to the reactive energy and the harmonic oscillator model, the relational expressions, between the infrared absorption and the Mn-O-Mn bond length and bo nd angel were studied. The infrared absorption near 600cm-1 relates t o the different lattice constant b, and the metal-insulator transformation tempe ratures (TMI) of the block material and the films differ much, those of the films being much lower than that of the block material and, at the same time, has something to do with the film thickness. The paper indicates that the stress in the LSMO films inducing the lattice constant change and then arousing the change of bond angel and JT effect is the main reason for the change of the transformation temperature.


Acta Physica Sinica. 2006 55(3): 1435-1440. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1435-1440. article doi:10.7498/aps.55.1435 10.7498/aps.55.1435 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1435 1435-1440
<![CDATA[Colossal magnetoresistance effect in the perovskite-type La1-xPrxMnO3 thin films]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1441

The oxide La1-xPrxMnO3 (x=0.1, 0.2) thin film s howing colossal magnetoresistance has been epitaxially grown on (100) SrTiO 3 single-crystal substrate by pulsed-laser deposition. The films have a pe rovskite structure and perform the colossal magnetoresistance effect with the ma ximum magnetoresistance ratio of 95% under the magnetic field of 5 T. The valenc e of Pr is confirmed as +4 through XPS. Therefore the epitaxial film is most lik ely an electron-doped colossal magnetoresistance fihn.


Acta Physica Sinica. 2006 55(3): 1441-1446. Published 2006-03-20 ]]>

The oxide La1-xPrxMnO3 (x=0.1, 0.2) thin film s howing colossal magnetoresistance has been epitaxially grown on (100) SrTiO 3 single-crystal substrate by pulsed-laser deposition. The films have a pe rovskite structure and perform the colossal magnetoresistance effect with the ma ximum magnetoresistance ratio of 95% under the magnetic field of 5 T. The valenc e of Pr is confirmed as +4 through XPS. Therefore the epitaxial film is most lik ely an electron-doped colossal magnetoresistance fihn.


Acta Physica Sinica. 2006 55(3): 1441-1446. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1441-1446. article doi:10.7498/aps.55.1441 10.7498/aps.55.1441 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1441 1441-1446
<![CDATA[Effect of Mn substitution on the structure and magnetic properties of Dy2AlFe16-xMnx compounds]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1447

The structural and magnetic properties have been investigated by means of X-ray diffraction and magnetization measurements. The Dy2AlFe16-xMnx compounds have a hexagonal Th2Ni17-type st ructure. The thermal expansion of Dy2AlFe16-xMnx (x=1 and 2) compounds have been investigated by X-ray dilatometry in the tempe rature range 104—647K. The results show that there is a thermal expansion anoma ly at low temperature and a negative thermal expansion near the Curie temperatur e. There exists a strong and anisotropic spontaneous magnetostriction in the mag netic state of Dy2AlFe16-xMnx compounds. The sp ontaneous volume magnetostrictive deformation at low temperature decreases with increasing x. The result of magnetization measurement shows that the Curie tempe rature and the spontaneous magnetization of Dy2AlFe16-xMnx compounds at 5K decrease rapidly with increasing x.


Acta Physica Sinica. 2006 55(3): 1447-1452. Published 2006-03-20 ]]>

The structural and magnetic properties have been investigated by means of X-ray diffraction and magnetization measurements. The Dy2AlFe16-xMnx compounds have a hexagonal Th2Ni17-type st ructure. The thermal expansion of Dy2AlFe16-xMnx (x=1 and 2) compounds have been investigated by X-ray dilatometry in the tempe rature range 104—647K. The results show that there is a thermal expansion anoma ly at low temperature and a negative thermal expansion near the Curie temperatur e. There exists a strong and anisotropic spontaneous magnetostriction in the mag netic state of Dy2AlFe16-xMnx compounds. The sp ontaneous volume magnetostrictive deformation at low temperature decreases with increasing x. The result of magnetization measurement shows that the Curie tempe rature and the spontaneous magnetization of Dy2AlFe16-xMnx compounds at 5K decrease rapidly with increasing x.


Acta Physica Sinica. 2006 55(3): 1447-1452. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1447-1452. article doi:10.7498/aps.55.1447 10.7498/aps.55.1447 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1447 1447-1452
<![CDATA[Room-temperature ferromagnetism in bulk CoxTi1-xO2-δ induced by the phase transformation in the hydrogenation sintering process]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1453

Paramagnetic (Co3O4)x/3(TiO2)1- x(03O4 and TiO2 from 700 ℃ to 1000 ℃ in air. X-ray diffraction (XRD) re sults showed that perovskite CoTiO3 existed in all samples. Anatase p hase was also detected in samples sintered at 700 ℃ and when sintering the mixt ure at above 900 ℃, rutile phase formed with anatase phase disappearing. All sa mples exhibited room-temperature ferromagnetism (RTFM) after being hydrogenated in 10% H2/Ar mixed atmosphere for 1 hour at 500 ℃. X-ray photoelect ron spectroscopy (XPS) showed that Co existed in the +2 formal oxidation state, and no Co clusters were detected. XRD showed that CoTiO3 disappeared and a new phase CoxTi1-xO2-δ formed after hyd rogenation. It is suggested that hydrogenation causes the phase transformation f rom CoTiO3 to CoxTi1-xO2-δ. RTFM of the sample originates from the intrinsic ferromagnetism of CoxTi1-xO2-δ. The exchange interaction between Co2+ occ urring with the phase transformation may be the essential reason for RTFM.


Acta Physica Sinica. 2006 55(3): 1453-1457. Published 2006-03-20 ]]>

Paramagnetic (Co3O4)x/3(TiO2)1- x(03O4 and TiO2 from 700 ℃ to 1000 ℃ in air. X-ray diffraction (XRD) re sults showed that perovskite CoTiO3 existed in all samples. Anatase p hase was also detected in samples sintered at 700 ℃ and when sintering the mixt ure at above 900 ℃, rutile phase formed with anatase phase disappearing. All sa mples exhibited room-temperature ferromagnetism (RTFM) after being hydrogenated in 10% H2/Ar mixed atmosphere for 1 hour at 500 ℃. X-ray photoelect ron spectroscopy (XPS) showed that Co existed in the +2 formal oxidation state, and no Co clusters were detected. XRD showed that CoTiO3 disappeared and a new phase CoxTi1-xO2-δ formed after hyd rogenation. It is suggested that hydrogenation causes the phase transformation f rom CoTiO3 to CoxTi1-xO2-δ. RTFM of the sample originates from the intrinsic ferromagnetism of CoxTi1-xO2-δ. The exchange interaction between Co2+ occ urring with the phase transformation may be the essential reason for RTFM.


Acta Physica Sinica. 2006 55(3): 1453-1457. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1453-1457. article doi:10.7498/aps.55.1453 10.7498/aps.55.1453 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1453 1453-1457
<![CDATA[Deposition of diamond-like carbon and analysis of ion energy in CH4 or CH4+Ar dielectric barrier discharge plasma]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1458

Diamond-like carbon (DLC) films were deposited by dielectric barrier discharge ( DBD) from CH4 or CH4 +Ar at pressure of several hundred Pa . The dependence of the film hardness on the product of p and d (p is the gas pr essure and the d is the discharge space) and Ar volume concentration (RAr) was investigated experimentally. The kinetic energies of CH+4 and Ar+ ions were analyzed theoretically based on the two-t emperature model for high reduced field E/n (the ratio of electric field strengt h to the gas number density), in which ions were assigned a temperature much hig her than the gas temperature, on the Langevin equation in other gas and on the B lanc law in mixed gases. The results showed that, 1) for CH4 DBD, whe n decreasing pd from 1.862×103Pa mm to 2.66×102Pa mm, th e kinetic energy of CH+4 increases from 5.4 to 163eV, whil e the hardness of deposited DLC films increases from 2.1 to 17.6 GPa. 2) For CH+4Ar DBD, when increasing Ar volume concentration from 20% to 83%, the kinetic energy of CH+4 increases from 69 to 92 eV, whereas the kinetic energy of Ar+ decreases from 93 to 72eV. The increase of film hardness with increasing Ar volume concentration up to 67% can be attributed to the increase of CH+4 kinetic energy. Howe ver, the impinging of energetic Ar+ on the film surface reduces the f ilm hardness owing to graphitization. For verification of the theoretical model on ion energy analysis, the kinetic energy of ions in H2 DBD were mea sured and compared with that from theoretical analysis.


Acta Physica Sinica. 2006 55(3): 1458-1463. Published 2006-03-20 ]]>

Diamond-like carbon (DLC) films were deposited by dielectric barrier discharge ( DBD) from CH4 or CH4 +Ar at pressure of several hundred Pa . The dependence of the film hardness on the product of p and d (p is the gas pr essure and the d is the discharge space) and Ar volume concentration (RAr) was investigated experimentally. The kinetic energies of CH+4 and Ar+ ions were analyzed theoretically based on the two-t emperature model for high reduced field E/n (the ratio of electric field strengt h to the gas number density), in which ions were assigned a temperature much hig her than the gas temperature, on the Langevin equation in other gas and on the B lanc law in mixed gases. The results showed that, 1) for CH4 DBD, whe n decreasing pd from 1.862×103Pa mm to 2.66×102Pa mm, th e kinetic energy of CH+4 increases from 5.4 to 163eV, whil e the hardness of deposited DLC films increases from 2.1 to 17.6 GPa. 2) For CH+4Ar DBD, when increasing Ar volume concentration from 20% to 83%, the kinetic energy of CH+4 increases from 69 to 92 eV, whereas the kinetic energy of Ar+ decreases from 93 to 72eV. The increase of film hardness with increasing Ar volume concentration up to 67% can be attributed to the increase of CH+4 kinetic energy. Howe ver, the impinging of energetic Ar+ on the film surface reduces the f ilm hardness owing to graphitization. For verification of the theoretical model on ion energy analysis, the kinetic energy of ions in H2 DBD were mea sured and compared with that from theoretical analysis.


Acta Physica Sinica. 2006 55(3): 1458-1463. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1458-1463. article doi:10.7498/aps.55.1458 10.7498/aps.55.1458 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1458 1458-1463
<![CDATA[Preparation and growth of SrBi4Ti4O15 ferroelectric thin film by sol-gel method]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1464

The stable strontium bismuth titanate (SBTi) precursor solution were prepared us ing strontium chloride, bismuth nitrate, tetrabulyl titranate as raw materials, with citric acid as complex agent, ethylene glycol as cross linker, and ethanol absolute, water, hydrochloric acid as solvents of tetrabulyl titranate, strontiu m chloride, bismuth nitrate, respectively. SBTi thin films with enhanced a-axis orientation were prepared on Pt/Ti/Si02/Si substrates by the Sol-Gel method. Wit h the aid of ESEM and XRD, the effects of annealing time and the number of coati ngs on microstructure crystallization and growth behavior of SBTi thin films wer e investigated. The results indicate that the pyrochlore phase was restrained su ccessfully by layer-by-layer rapid thermal annealing method. The crystallization of the film was enhanced with the increase of coating number. Because of the an isotropic growth of SBTi crystals and the suppressed growth in (119) direction b y the thickness of single-annealed layer, the intensity of (200) and (119) peaks increase with the increase of layers, and the former increase more quickly.Howe ver, the intensity of (00l) peak decreased with the increase of layers, so the r elative intensity of (200) [I(200)/I(119),I(200)/I(0010)] and (119) [I(119)/ I(0010)] increases with the increase of layers.


Acta Physica Sinica. 2006 55(3): 1464-1471. Published 2006-03-20 ]]>

The stable strontium bismuth titanate (SBTi) precursor solution were prepared us ing strontium chloride, bismuth nitrate, tetrabulyl titranate as raw materials, with citric acid as complex agent, ethylene glycol as cross linker, and ethanol absolute, water, hydrochloric acid as solvents of tetrabulyl titranate, strontiu m chloride, bismuth nitrate, respectively. SBTi thin films with enhanced a-axis orientation were prepared on Pt/Ti/Si02/Si substrates by the Sol-Gel method. Wit h the aid of ESEM and XRD, the effects of annealing time and the number of coati ngs on microstructure crystallization and growth behavior of SBTi thin films wer e investigated. The results indicate that the pyrochlore phase was restrained su ccessfully by layer-by-layer rapid thermal annealing method. The crystallization of the film was enhanced with the increase of coating number. Because of the an isotropic growth of SBTi crystals and the suppressed growth in (119) direction b y the thickness of single-annealed layer, the intensity of (200) and (119) peaks increase with the increase of layers, and the former increase more quickly.Howe ver, the intensity of (00l) peak decreased with the increase of layers, so the r elative intensity of (200) [I(200)/I(119),I(200)/I(0010)] and (119) [I(119)/ I(0010)] increases with the increase of layers.


Acta Physica Sinica. 2006 55(3): 1464-1471. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1464-1471. article doi:10.7498/aps.55.1464 10.7498/aps.55.1464 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1464 1464-1471
<![CDATA[Growth and properties of the c-axis oriented Bi3.15Nd0.75 Ti3O12 ferroelectric multi-layer thin films on silicon substrates]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1472

The c-axis oriented Bi3.15Nd0.75Ti3O12(BNT) ferroelectric thin films were grown on Si(100) substrates by pulsed lase r deposition with La0.5Sr0.5CoO3/CeO2/Y0.18Zr0.91O2.01 multi-heterostructure as buf fer layer. X-ray diffraction and scanning electron microscopy were used to deter mine the microstructure, orientation and morphology of the multi-layer films. Th e influence of deposition temperatures and the partial oxygen pressure on the mi crostructure, orientation and morphology of the BNT films were investigated and the optimal deposition parameters were determined. The BNT multi-layer thin film s deposited under optimal condition have good electric properties. The C-V patte rn of the BNT multilayer thin films deposited under optimal deposition condition s has the typical butterfly-like shape, suggesting that the films have good pola rization-reversion storage properties. The correlation between the ferroelectric properties and the orientations of the BNT films is discussed.


Acta Physica Sinica. 2006 55(3): 1472-1478. Published 2006-03-20 ]]>

The c-axis oriented Bi3.15Nd0.75Ti3O12(BNT) ferroelectric thin films were grown on Si(100) substrates by pulsed lase r deposition with La0.5Sr0.5CoO3/CeO2/Y0.18Zr0.91O2.01 multi-heterostructure as buf fer layer. X-ray diffraction and scanning electron microscopy were used to deter mine the microstructure, orientation and morphology of the multi-layer films. Th e influence of deposition temperatures and the partial oxygen pressure on the mi crostructure, orientation and morphology of the BNT films were investigated and the optimal deposition parameters were determined. The BNT multi-layer thin film s deposited under optimal condition have good electric properties. The C-V patte rn of the BNT multilayer thin films deposited under optimal deposition condition s has the typical butterfly-like shape, suggesting that the films have good pola rization-reversion storage properties. The correlation between the ferroelectric properties and the orientations of the BNT films is discussed.


Acta Physica Sinica. 2006 55(3): 1472-1478. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1472-1478. article doi:10.7498/aps.55.1472 10.7498/aps.55.1472 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1472 1472-1478
<![CDATA[Effect of radiation trapping on spectroscopic properties of Er3+-doped oxide glasses]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1479

The absorption spectra, fluorescence spectra and the lifetimes of 4I13/2 level of Er3+-doped phosphate and tellurite glasses ha ve been measured for sample with different concentrations and thickness. The abs orption cross-section (σa), emission cross-section(σe), spontaneous emission probability(Arad), radiative lifetime(τrad ) and quantum efficiency(η) of fluorescence around 1.53 μm of Er3+-doped phosphate and tellurite glasses were determined. The effect of radia tion trapping on the spectral properties and parameters of Er3+-doped tellurite and phosphate glasses has been investigated. It was found that radiat ion trapping exists generally in erbium-doped glass hosts, even at low Er3+ -doping concentration (0.1 mol% Er2O3). Due to radia tion trapping, the values of the τrad of the Er3+∶4 I13/2 level in tellurite glasses increased about 11%—37% with the sample thickness and erbium doping concentration, while in phosphate glasse s τrad increased by 6%—17%. The full-width at half maximum (FWHM)of fluorescence in tellurite glasses increased about 15%—64%, with 11%—55% for p hosphate glasses. It caused a high overestimation on the figure of merits (FOM) for amplifier bandwidth (σe×FWHM). The spectral overlap between the emission and absorption spectra in 1.53 μm band is relatively larger in tellur ite than in phosphate glasses, and values of the emission cross-section in tellu rite glasses are larger than that in phosphate glasses. Consequently, the radiat ion trapping in tellurite glasses is more severel than that in phosphate glasses .


Acta Physica Sinica. 2006 55(3): 1479-1485. Published 2006-03-20 ]]>

The absorption spectra, fluorescence spectra and the lifetimes of 4I13/2 level of Er3+-doped phosphate and tellurite glasses ha ve been measured for sample with different concentrations and thickness. The abs orption cross-section (σa), emission cross-section(σe), spontaneous emission probability(Arad), radiative lifetime(τrad ) and quantum efficiency(η) of fluorescence around 1.53 μm of Er3+-doped phosphate and tellurite glasses were determined. The effect of radia tion trapping on the spectral properties and parameters of Er3+-doped tellurite and phosphate glasses has been investigated. It was found that radiat ion trapping exists generally in erbium-doped glass hosts, even at low Er3+ -doping concentration (0.1 mol% Er2O3). Due to radia tion trapping, the values of the τrad of the Er3+∶4 I13/2 level in tellurite glasses increased about 11%—37% with the sample thickness and erbium doping concentration, while in phosphate glasse s τrad increased by 6%—17%. The full-width at half maximum (FWHM)of fluorescence in tellurite glasses increased about 15%—64%, with 11%—55% for p hosphate glasses. It caused a high overestimation on the figure of merits (FOM) for amplifier bandwidth (σe×FWHM). The spectral overlap between the emission and absorption spectra in 1.53 μm band is relatively larger in tellur ite than in phosphate glasses, and values of the emission cross-section in tellu rite glasses are larger than that in phosphate glasses. Consequently, the radiat ion trapping in tellurite glasses is more severel than that in phosphate glasses .


Acta Physica Sinica. 2006 55(3): 1479-1485. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1479-1485. article doi:10.7498/aps.55.1479 10.7498/aps.55.1479 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1479 1479-1485
<![CDATA[Upconversion emission properties of Er3+ in fluoride (halide) phosphate tellurite glasses]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1486

The absorption and upconversion spectra of Er3+-doped fluoride (halid e) phosphate tellurite glasses were investigated for the first time, and the upc onversion mechanisms were studied. Strong red and green upconversion luminescenc e were observed under 975nm laser diode excitation at room temperature. When PbF 2 is partially replaced by PbCl2 gradually, the intensity of red emission decreases, while the green emission intensity changes only sligh tly. When ZnF2 is replaced by 5mol% ZnCl2, both red and gr een emissions intensity are enhanced obviously.


Acta Physica Sinica. 2006 55(3): 1486-1490. Published 2006-03-20 ]]>

The absorption and upconversion spectra of Er3+-doped fluoride (halid e) phosphate tellurite glasses were investigated for the first time, and the upc onversion mechanisms were studied. Strong red and green upconversion luminescenc e were observed under 975nm laser diode excitation at room temperature. When PbF 2 is partially replaced by PbCl2 gradually, the intensity of red emission decreases, while the green emission intensity changes only sligh tly. When ZnF2 is replaced by 5mol% ZnCl2, both red and gr een emissions intensity are enhanced obviously.


Acta Physica Sinica. 2006 55(3): 1486-1490. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1486-1490. article doi:10.7498/aps.55.1486 10.7498/aps.55.1486 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1486 1486-1490
<![CDATA[Bicrystalline zinc oxide nanocombs]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1491

Bicrystalline ZnO nanocombs have been prepared by zinc powder evaporation proces s at 650℃. The structure of bicrystalline ZnO nanocombs was characterized by XR D, HTEM, SAD, etc., which indicate that the as-synthesized sample are composed of two crystals that form a twin structure parallel to the (1 1 3) plane with th e growth direction of the branching nanowires and the main stems closely paralle l to〈0 0 0 1〉 and〈0 1 1 0〉,respectively. Due to the unique twin structures, both sides of the main stems could be Zn-terminated ZnO (0 0 0 1) polar surface s, which are chemically active. Therefore the aligned branching nanowires can be grown from both sides of the main stems, which is consistent with the structure of the bicrystalline nanomaterials we have obtained. The growth of bicrystallin e ZnO nanocombs bears direct evidence to the polar-surface dominated growth mech anism of the ZnO nanomaterials.


Acta Physica Sinica. 2006 55(3): 1491-1496. Published 2006-03-20 ]]>

Bicrystalline ZnO nanocombs have been prepared by zinc powder evaporation proces s at 650℃. The structure of bicrystalline ZnO nanocombs was characterized by XR D, HTEM, SAD, etc., which indicate that the as-synthesized sample are composed of two crystals that form a twin structure parallel to the (1 1 3) plane with th e growth direction of the branching nanowires and the main stems closely paralle l to〈0 0 0 1〉 and〈0 1 1 0〉,respectively. Due to the unique twin structures, both sides of the main stems could be Zn-terminated ZnO (0 0 0 1) polar surface s, which are chemically active. Therefore the aligned branching nanowires can be grown from both sides of the main stems, which is consistent with the structure of the bicrystalline nanomaterials we have obtained. The growth of bicrystallin e ZnO nanocombs bears direct evidence to the polar-surface dominated growth mech anism of the ZnO nanomaterials.


Acta Physica Sinica. 2006 55(3): 1491-1496. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1491-1496. article doi:10.7498/aps.55.1491 10.7498/aps.55.1491 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1491 1491-1496
<![CDATA[Effect of excitation frequency on microcrystalline silicon materials prepared by VHF-PECVD]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1497

Hydrogenated microcrystalline silicon (μc-Si:H) materials was prepared by plasm a enhanced chemical vapor deposition (PECVD) at silane concentration 6% and 7% w ith changing excitation frequency (40—70MHz). Relationship between excitation f requency and electrical, structural characteristics and deposition rate of the m aterials was studied. The results indicate that the crystalline volume fraction (Xc) decrease firstly and then increase with the increase of excitati on frequency. But the photosensitivity and the deposition rate be have adversely with the change of excitation frequency. The reason of change of structure and deposition rate of thin films with excitation frequency was studied by optical e mission spectroscopy.


Acta Physica Sinica. 2006 55(3): 1497-1501. Published 2006-03-20 ]]>

Hydrogenated microcrystalline silicon (μc-Si:H) materials was prepared by plasm a enhanced chemical vapor deposition (PECVD) at silane concentration 6% and 7% w ith changing excitation frequency (40—70MHz). Relationship between excitation f requency and electrical, structural characteristics and deposition rate of the m aterials was studied. The results indicate that the crystalline volume fraction (Xc) decrease firstly and then increase with the increase of excitati on frequency. But the photosensitivity and the deposition rate be have adversely with the change of excitation frequency. The reason of change of structure and deposition rate of thin films with excitation frequency was studied by optical e mission spectroscopy.


Acta Physica Sinica. 2006 55(3): 1497-1501. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1497-1501. article doi:10.7498/aps.55.1497 10.7498/aps.55.1497 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1497 1497-1501
<![CDATA[Numerical simulation of solute segregation patterns for a binary alloy using phase-field approach]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1502

The dependence of denderitic patterns and solute segregation on solid diffusivit y Ds is studied using a phase-field model which incorporates concentr ation field for Ni-Cu binary alloy dendritic growth. The computed results indica te that with the decrease of solid diffusivity Ds, the smaller become s the thickness of the solute diffusion layer ahead of the interface, which is a dvantageous to the growth of the sidebranching, and the more developed the side- branches. The smaller the solid diffusivity Ds, the more acutely the solute concentration in solid phase fluctuates. With the increment of solid diff usivity Ds, the fluctuations of solute concentration in solid phase a re reduced accordingly. An increased level of solid diffusivity Ds re duces the severity of microsegregation.


Acta Physica Sinica. 2006 55(3): 1502-1507. Published 2006-03-20 ]]>

The dependence of denderitic patterns and solute segregation on solid diffusivit y Ds is studied using a phase-field model which incorporates concentr ation field for Ni-Cu binary alloy dendritic growth. The computed results indica te that with the decrease of solid diffusivity Ds, the smaller become s the thickness of the solute diffusion layer ahead of the interface, which is a dvantageous to the growth of the sidebranching, and the more developed the side- branches. The smaller the solid diffusivity Ds, the more acutely the solute concentration in solid phase fluctuates. With the increment of solid diff usivity Ds, the fluctuations of solute concentration in solid phase a re reduced accordingly. An increased level of solid diffusivity Ds re duces the severity of microsegregation.


Acta Physica Sinica. 2006 55(3): 1502-1507. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1502-1507. article doi:10.7498/aps.55.1502 10.7498/aps.55.1502 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1502 1502-1507
<![CDATA[Microstructure of TiNi shape memory alloy films made of sputter-deposited Ni/Ti multilayers]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1508

Phase depth profile in TiNi shape memory alloy films is studied by the combinati on of grazing-incidence X-ray diffraction and X-ray reflectivity measurement. Th e film is made from sputter-deposited Ni/Ti multilayers. At room temperature, bo th the phase depth profile and element depth profile are not uniform, and both h ave multilayer structure. There is a three-phase mixture region consisting of Ti 3Ni4 precipitates, martensite and a little of austenite ne ar the free surface. A uniform martensite phase is formed near the substrate. Di ffusion and reaction take place between film and substrate. The simulation resul t of X-ray reflectivity shows that the results of film microstructure analysis a re reasonable. It is the kinetic factors that mainly cause the ununiformity of p hase depth profile in the film.


Acta Physica Sinica. 2006 55(3): 1508-1511. Published 2006-03-20 ]]>

Phase depth profile in TiNi shape memory alloy films is studied by the combinati on of grazing-incidence X-ray diffraction and X-ray reflectivity measurement. Th e film is made from sputter-deposited Ni/Ti multilayers. At room temperature, bo th the phase depth profile and element depth profile are not uniform, and both h ave multilayer structure. There is a three-phase mixture region consisting of Ti 3Ni4 precipitates, martensite and a little of austenite ne ar the free surface. A uniform martensite phase is formed near the substrate. Di ffusion and reaction take place between film and substrate. The simulation resul t of X-ray reflectivity shows that the results of film microstructure analysis a re reasonable. It is the kinetic factors that mainly cause the ununiformity of p hase depth profile in the film.


Acta Physica Sinica. 2006 55(3): 1508-1511. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1508-1511. article doi:10.7498/aps.55.1508 10.7498/aps.55.1508 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1508 1508-1511
<![CDATA[Memory characteristics of metal-ferroelectric-semiconductor field-effect-transistors with Ag/Bi4Ti3O12/p-Si gate]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1512

Metal-ferroelectric-semiconductor field-effect-transistors (FFETs) with Ag/Bi4Ti3O12/p-Si gate were fabricated using the high q uality Bi4Ti3O12 on p-Si substrates prepared by Sol-Gel technique. The phase structure characteristics of Bi4Ti 3O12 films, the interface characteristics of ferroelectric/Si a nd the memory characteristics of the FFETs were investigated. Bi4Ti 3O12 films with high preferred c-axis-orientation are obta ined at appropriate annealing temperature which helps to improve the interface c haracteristics of ferroelectric/Si. The C-V hysteresis curves with clockwise loo ps prove that the FFETs could realize a memory effect due to the ferroelectric p olarization of Bi4Ti3O12 films, and the capacit ance decay of 11% in 16 hours indicates that the FFETs have good polarization ch arge retention. The counter-clockwise Ids-VG hysterisis cu rve of the FFETs demonstrates that the channel current is modulated by the ferro electric polarization of Bi4Ti3O12 films.


Acta Physica Sinica. 2006 55(3): 1512-1516. Published 2006-03-20 ]]>

Metal-ferroelectric-semiconductor field-effect-transistors (FFETs) with Ag/Bi4Ti3O12/p-Si gate were fabricated using the high q uality Bi4Ti3O12 on p-Si substrates prepared by Sol-Gel technique. The phase structure characteristics of Bi4Ti 3O12 films, the interface characteristics of ferroelectric/Si a nd the memory characteristics of the FFETs were investigated. Bi4Ti 3O12 films with high preferred c-axis-orientation are obta ined at appropriate annealing temperature which helps to improve the interface c haracteristics of ferroelectric/Si. The C-V hysteresis curves with clockwise loo ps prove that the FFETs could realize a memory effect due to the ferroelectric p olarization of Bi4Ti3O12 films, and the capacit ance decay of 11% in 16 hours indicates that the FFETs have good polarization ch arge retention. The counter-clockwise Ids-VG hysterisis cu rve of the FFETs demonstrates that the channel current is modulated by the ferro electric polarization of Bi4Ti3O12 films.


Acta Physica Sinica. 2006 55(3): 1512-1516. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1512-1516. article doi:10.7498/aps.55.1512 10.7498/aps.55.1512 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1512 1512-1516
<![CDATA[Etching effects of low energy argon ion beam on porous anodic aluminum oxide membranes]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1517

Porous anodic aluminum oxide (AAO) membranes were sputtered by 500eV argon ion ( Ar+) beam. Scanning electron microscopy and atomic force microscopy i mages show that not only the barrier layer of AAO can be easily removed by Ar+ beam sputtering, but also several categories of surface morphologies w ere got by changing the incidence parameters. For instance, off-normal incidence bombardment results in ripple formation on the surface of AAO and off-normal in cidence during smple stage rotation leads to AAO surface smoothing. Theory of ri pple formation and evolution on amorphous substrate under ion beam irradiation d eveloped by Bradley and Harper is used to interpret the characteristics of rippl es on AAO surface.


Acta Physica Sinica. 2006 55(3): 1517-1522. Published 2006-03-20 ]]>

Porous anodic aluminum oxide (AAO) membranes were sputtered by 500eV argon ion ( Ar+) beam. Scanning electron microscopy and atomic force microscopy i mages show that not only the barrier layer of AAO can be easily removed by Ar+ beam sputtering, but also several categories of surface morphologies w ere got by changing the incidence parameters. For instance, off-normal incidence bombardment results in ripple formation on the surface of AAO and off-normal in cidence during smple stage rotation leads to AAO surface smoothing. Theory of ri pple formation and evolution on amorphous substrate under ion beam irradiation d eveloped by Bradley and Harper is used to interpret the characteristics of rippl es on AAO surface.


Acta Physica Sinica. 2006 55(3): 1517-1522. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1517-1522. article doi:10.7498/aps.55.1517 10.7498/aps.55.1517 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1517 1517-1522
<![CDATA[Influence of weak magnetic field on growth morphology of Zn branched electrodeposits]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1523

The influence of a weak magnetic field on the microstructure of the Zn electrode posits prepared in a thin concentric electrode cell is investigated. Mechanism o f the effect of the magnetohydrodynamic (MHD) flow on the morphological transiti on is proposed through experimental evidences. 1) In the early growth phase of a crystallite, the unbalanced force caused by the MHD flow on the crystallite, wh ich suspends in the electrolyte close to the previous branch, rotates its prefer ential growth orientation towards the downstream of the MHD flow; 2) A stable co ncentration profile is formed in the vicinity of the electrodeposits by the MHD flow. After the crystallite grows large enough to stick on its previous branch, and the concentration of the electrolyte is high enough for both the primary bra nch and its secondary branches, the single-crystalline dendrites will grow strai ght. But if the concentration of the electrolyte is small, the secondary branche s crowd to the side facing the upstream of the MHD flow and the primary branch i s forced to bend towards the downstream of the MHD flow. A spiral structure in t he branched electrodeposits grown in a magnetic field is formed by this mechanis m.


Acta Physica Sinica. 2006 55(3): 1523-1528. Published 2006-03-20 ]]>

The influence of a weak magnetic field on the microstructure of the Zn electrode posits prepared in a thin concentric electrode cell is investigated. Mechanism o f the effect of the magnetohydrodynamic (MHD) flow on the morphological transiti on is proposed through experimental evidences. 1) In the early growth phase of a crystallite, the unbalanced force caused by the MHD flow on the crystallite, wh ich suspends in the electrolyte close to the previous branch, rotates its prefer ential growth orientation towards the downstream of the MHD flow; 2) A stable co ncentration profile is formed in the vicinity of the electrodeposits by the MHD flow. After the crystallite grows large enough to stick on its previous branch, and the concentration of the electrolyte is high enough for both the primary bra nch and its secondary branches, the single-crystalline dendrites will grow strai ght. But if the concentration of the electrolyte is small, the secondary branche s crowd to the side facing the upstream of the MHD flow and the primary branch i s forced to bend towards the downstream of the MHD flow. A spiral structure in t he branched electrodeposits grown in a magnetic field is formed by this mechanis m.


Acta Physica Sinica. 2006 55(3): 1523-1528. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1523-1528. article doi:10.7498/aps.55.1523 10.7498/aps.55.1523 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1523 1523-1528
<![CDATA[Measurement of nitrous acid and retrieval of aerosol parameters with differential optical absorption spectroscopy]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1529

Differential optical absorption spectroscopy (DOAS) is a spectroscopic technique which can be used to monitor many kinds of air pollutants simultaneously. In th is paper, in situ measurement of nitrous acid and retrieval of aerosol parameter s in a fixed wavelength range (307 nm—380 nm) were performed with DOAS system d eveloped by our laboratory. The measurements of HONO concentration were more acc urate using the NO2 standard absorption cross section measured by our selves a nd aerosol parameters were retrieved successfully in a shorter wavelength range.


Acta Physica Sinica. 2006 55(3): 1529-1533. Published 2006-03-20 ]]>

Differential optical absorption spectroscopy (DOAS) is a spectroscopic technique which can be used to monitor many kinds of air pollutants simultaneously. In th is paper, in situ measurement of nitrous acid and retrieval of aerosol parameter s in a fixed wavelength range (307 nm—380 nm) were performed with DOAS system d eveloped by our laboratory. The measurements of HONO concentration were more acc urate using the NO2 standard absorption cross section measured by our selves a nd aerosol parameters were retrieved successfully in a shorter wavelength range.


Acta Physica Sinica. 2006 55(3): 1529-1533. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1529-1533. article doi:10.7498/aps.55.1529 10.7498/aps.55.1529 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1529 1529-1533
<![CDATA[Simulation of effect of atomic process on poloidal CXRS measurement]]> //m.suprmerch.com/en/article/doi/10.7498/aps.55.1534

With consideration of the effects of atomic process, a simple code modeling the correction to poloidal charge-exchange recombination spectroscopy (CXRS) measure ment is developed. The simulation results show that the measured poloidal veloci ty shift is overestimated in the ion diamagnetic drift direction and the apparen t ion temperature is underestimated because of the effects of energy-dependent e mission rate and finite lifetime of excited ions. This deviation will be more ob vious with the increase of temperature or magnetic field. The contributions from gradients of density and temperature are negligible compared to that from the a tomic process.


Acta Physica Sinica. 2006 55(3): 1534-1538. Published 2006-03-20 ]]>

With consideration of the effects of atomic process, a simple code modeling the correction to poloidal charge-exchange recombination spectroscopy (CXRS) measure ment is developed. The simulation results show that the measured poloidal veloci ty shift is overestimated in the ion diamagnetic drift direction and the apparen t ion temperature is underestimated because of the effects of energy-dependent e mission rate and finite lifetime of excited ions. This deviation will be more ob vious with the increase of temperature or magnetic field. The contributions from gradients of density and temperature are negligible compared to that from the a tomic process.


Acta Physica Sinica. 2006 55(3): 1534-1538. Published 2006-03-20 ]]>
2006-02-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2006 55(3): 1534-1538. article doi:10.7498/aps.55.1534 10.7498/aps.55.1534 Acta Physica Sinica 55 3 2006-03-20 //m.suprmerch.com/en/article/doi/10.7498/aps.55.1534 1534-1538