A discussion on the q-oscillator system and the algebra Hq(4) is presented, emphasizing the case of |q| = 1 in particular. A remarkable connection between algebras SUq(2) and Hq(4) is given. The single q-oscillator system is solved and shown to be analogous to the parafermion-(PF), with the specific cases analogous to 2nd and 3rd order PF's discussed in detail. The properties of the representations of Hq(4) and a finite chain model of q-oscillators are discussed-
A discussion on the q-oscillator system and the algebra Hq(4) is presented, emphasizing the case of |q| = 1 in particular. A remarkable connection between algebras SUq(2) and Hq(4) is given. The single q-oscillator system is solved and shown to be analogous to the parafermion-(PF), with the specific cases analogous to 2nd and 3rd order PF's discussed in detail. The properties of the representations of Hq(4) and a finite chain model of q-oscillators are discussed-
The mean free path of the FHP hydrodynamical models is calculated. The calculations show that the mean free path is approximate to a constant after more than 60 collisions and is a minimum, which is corresponding to the maximum of Reynolds' number, when particle density is 0.25. In addition, the difference between the FHP models and the molecular dynamic models is showed clearly.
The mean free path of the FHP hydrodynamical models is calculated. The calculations show that the mean free path is approximate to a constant after more than 60 collisions and is a minimum, which is corresponding to the maximum of Reynolds' number, when particle density is 0.25. In addition, the difference between the FHP models and the molecular dynamic models is showed clearly.
The K-structures of the CSM wave functions in 164Er96 and 166Er98 were analyzed in the represention, the bases of which are characterized by the quantum numbers N,π,r,v,K,E1. The K-structure becomes complex as ω increases and the system becomes axially asymmetric. The calculation shows that the K-structure of the yrast band in 164Er96 is very similar to that in 166Er98, but the K-structure of the yrare band in 164Er96 is quite different from that in 166Er98.
The K-structures of the CSM wave functions in 164Er96 and 166Er98 were analyzed in the represention, the bases of which are characterized by the quantum numbers N,π,r,v,K,E1. The K-structure becomes complex as ω increases and the system becomes axially asymmetric. The calculation shows that the K-structure of the yrast band in 164Er96 is very similar to that in 166Er98, but the K-structure of the yrare band in 164Er96 is quite different from that in 166Er98.
Starting from the space-translated version of Schr?dinger equation of H-atoms in the laser fields with circular polarization, the features of the dressed coulomb potential are analyzed, a small expansion parameter is found and a perturbation-iteration method is presented. Then the zero to second order approximation equations of Floquet-Schr?dinger equation are derived It is shown that the above-mentioned expansion in the small parameter makes the iteration method to give a correct result. Furthermore, the advantages of the approach are qualitatively displayed by a brief comparison of the results given in this paper with the previous results.
Starting from the space-translated version of Schr?dinger equation of H-atoms in the laser fields with circular polarization, the features of the dressed coulomb potential are analyzed, a small expansion parameter is found and a perturbation-iteration method is presented. Then the zero to second order approximation equations of Floquet-Schr?dinger equation are derived It is shown that the above-mentioned expansion in the small parameter makes the iteration method to give a correct result. Furthermore, the advantages of the approach are qualitatively displayed by a brief comparison of the results given in this paper with the previous results.
The Above-threshold-ionization(ATI) Spectrum of electrons produced by multiphoton absorption of atom has been obtained with spatial Gauss and temporal Sech shape of the incident laser pulse. It is found that our model can explain many phenomena such as peak suppression and switching. In addition, what is more important is that we can explain the red shift of the peaks decreases to zero gradually, as the pulse width changes from short to long pulse regime.
The Above-threshold-ionization(ATI) Spectrum of electrons produced by multiphoton absorption of atom has been obtained with spatial Gauss and temporal Sech shape of the incident laser pulse. It is found that our model can explain many phenomena such as peak suppression and switching. In addition, what is more important is that we can explain the red shift of the peaks decreases to zero gradually, as the pulse width changes from short to long pulse regime.
Aluminium targets were irradiated by line focus laser. We observed spectra of high ioni-zation states in the range of VUV. By means of Cowan program for atomic energy level, we caleulated the wavelength and gf value of different ionization state and identified 140 spectra lines.82 new spectra lines were found.
Aluminium targets were irradiated by line focus laser. We observed spectra of high ioni-zation states in the range of VUV. By means of Cowan program for atomic energy level, we caleulated the wavelength and gf value of different ionization state and identified 140 spectra lines.82 new spectra lines were found.
Rare earth elements Tb, Er and Lu were bombarded by protons with energies of 0.2-1.2 MeV, L-subshell ionization cross sections were obtained. Experimental ionization cross sections were compared with the predictions of the ECPSSR theory.
Rare earth elements Tb, Er and Lu were bombarded by protons with energies of 0.2-1.2 MeV, L-subshell ionization cross sections were obtained. Experimental ionization cross sections were compared with the predictions of the ECPSSR theory.
Taking into account the location, size and also the shape of the defector, we calculated the values of the selectivity and the effective transmittance solid angle of the hexapole magnet system, and compared the results with those of the previous method. The dependence of the selectivity and the effective transmittance solid angle on various experimental parameters, and the ways to improve the performance of the hexapole magnet system were discussed. The selectivity was measured by laser-induced fluorescence (LIF) and the results were in good agreement with the theoretical ones.
Taking into account the location, size and also the shape of the defector, we calculated the values of the selectivity and the effective transmittance solid angle of the hexapole magnet system, and compared the results with those of the previous method. The dependence of the selectivity and the effective transmittance solid angle on various experimental parameters, and the ways to improve the performance of the hexapole magnet system were discussed. The selectivity was measured by laser-induced fluorescence (LIF) and the results were in good agreement with the theoretical ones.
According to Kukhtarev photorefractive theory, spontaneous generated moving refractive-index phase grating and strong backward photorefractive scattering produced by the phase grating in LiNbO3: Fe crystals are analysed.
According to Kukhtarev photorefractive theory, spontaneous generated moving refractive-index phase grating and strong backward photorefractive scattering produced by the phase grating in LiNbO3: Fe crystals are analysed.
In case the speed v of the atoms flying scross the cavity can be exactly adjusted, the light field originally in the cavity may be built into amplitude-squeezed state by adjusting the speed v to the preassigned value. It is also capable to make the photon distribution to have several peaks.
In case the speed v of the atoms flying scross the cavity can be exactly adjusted, the light field originally in the cavity may be built into amplitude-squeezed state by adjusting the speed v to the preassigned value. It is also capable to make the photon distribution to have several peaks.
A scheme is suggested in this paper, by which squeezed state light can be radiated from lasers directly via non-degenerate backward four wave mixing in laser cavities. Full quantum theory calculations predict that the output light shows good squeezing.
A scheme is suggested in this paper, by which squeezed state light can be radiated from lasers directly via non-degenerate backward four wave mixing in laser cavities. Full quantum theory calculations predict that the output light shows good squeezing.
A finite element algorithm is used to analyze the process of floating zone Gystal growth under microgravity. The effect of phase change convection coupled with surface tension convection is considered. The results show that the rate of crystal growth is very important. The single-crystal-melt interface is steeper than the feed-melt interface during the process of crystal growth. When the rate exceeds a critical value, the Marangoni vortex nearby the feed-melt interface will become so large that a secondary vortex exists.
A finite element algorithm is used to analyze the process of floating zone Gystal growth under microgravity. The effect of phase change convection coupled with surface tension convection is considered. The results show that the rate of crystal growth is very important. The single-crystal-melt interface is steeper than the feed-melt interface during the process of crystal growth. When the rate exceeds a critical value, the Marangoni vortex nearby the feed-melt interface will become so large that a secondary vortex exists.
Progressive waves expressed by rational combination of elliptic functions in general and solitary waves, solitons and kinks in special cases are found as solutions to various nonlinear wave equations.
Progressive waves expressed by rational combination of elliptic functions in general and solitary waves, solitons and kinks in special cases are found as solutions to various nonlinear wave equations.
The electronic characteristics of GaAs grown on Si by molecular beam epitaxy(MBE) has been examined by studying the diode characteristics and deep level transient spectroscopy (DLTS) of Schottky barriers. l-V characteristics of samples show the existence large leakage current. Post-growth rapid thermal annealing(RTA)has been found to be able to significantly improve the diode behaviour. The reverse current in the as-grown material shows a very weak temperature dependence, indicating that its origin is not thermoionic emission or generation-recombination currents. We think that a large part of this current is due to defect-assisted tunneling, which is reduced by RTA. DLTS spectra show that Ec-0.41eV and Ec-0.57eV electron traps are observable. The former is located near the GaAs-Si interface probably, the latter relates to the well-known electron trap M5 typical of MBE GaAs.
The electronic characteristics of GaAs grown on Si by molecular beam epitaxy(MBE) has been examined by studying the diode characteristics and deep level transient spectroscopy (DLTS) of Schottky barriers. l-V characteristics of samples show the existence large leakage current. Post-growth rapid thermal annealing(RTA)has been found to be able to significantly improve the diode behaviour. The reverse current in the as-grown material shows a very weak temperature dependence, indicating that its origin is not thermoionic emission or generation-recombination currents. We think that a large part of this current is due to defect-assisted tunneling, which is reduced by RTA. DLTS spectra show that Ec-0.41eV and Ec-0.57eV electron traps are observable. The former is located near the GaAs-Si interface probably, the latter relates to the well-known electron trap M5 typical of MBE GaAs.
On the basis of having proved that there exists the Anderson transition zone in the Aubry model of one-dimensional incommensurate systeme, we further study the relation between the Anderson transition zone and energy. Our numerical results indicate that the Anderson transition zone of the eigenstates in higher energy region is located in the range of lower values of the potential strength V, while, the Anderson transition zone of the eigenstates in lower energy region is located in the range of higher values of V.
On the basis of having proved that there exists the Anderson transition zone in the Aubry model of one-dimensional incommensurate systeme, we further study the relation between the Anderson transition zone and energy. Our numerical results indicate that the Anderson transition zone of the eigenstates in higher energy region is located in the range of lower values of the potential strength V, while, the Anderson transition zone of the eigenstates in lower energy region is located in the range of higher values of V.
In the present work, adsorptions of Li,Na,K,Cs on GaAs(llO) surface are studied. Both the ideal and the relaxed surface are considered. The calculations are carried out by using the charge self-consistent EHT method with a cluster model. The results indicate that the surface atoms tend to the ideal configuration after adsorption, and the alkali atom lies at the symmetric plane perpendicular to the surface and crossing the surface Ga atoms along the [001] direction. The Fermilevel is located about 0.7eV above the valence band maximum, which is contributed by the interaction between the surface Ga atoms and the alkali atom, while in the valence band, the alkali atom is bonded mostly with the surface As atoms.
In the present work, adsorptions of Li,Na,K,Cs on GaAs(llO) surface are studied. Both the ideal and the relaxed surface are considered. The calculations are carried out by using the charge self-consistent EHT method with a cluster model. The results indicate that the surface atoms tend to the ideal configuration after adsorption, and the alkali atom lies at the symmetric plane perpendicular to the surface and crossing the surface Ga atoms along the [001] direction. The Fermilevel is located about 0.7eV above the valence band maximum, which is contributed by the interaction between the surface Ga atoms and the alkali atom, while in the valence band, the alkali atom is bonded mostly with the surface As atoms.
This paper study the delay of destructive breakdown and its mechanism on SiO2 films by TCE treatment. The result show that the breakdown current capacity increase with increasing the TCE flow-rate, treatment time and temperature, and reducing the oxygen partial pressure. However, excessive quantity of the TCE flow-rate and prolonging of treatment time make the breakdown characteristics degradation begin to appear. The results also indicate, the increment of breakdown current capacity is associate with the increment of density of electron trap in SiO2 films. In this paper, we propose a breakdown model of 'low barrier point-electrical field enhanced' which involve three processes of mutual reinforcement, and consider for the first time the effect of H2O in TCE oxidation on the breakdown characteristics. The restrained function of electron trap on electrical field enhanced in low barrier point is quoted, and analyze the mechanism for delay of destructive breakdown in TCE oxides.
This paper study the delay of destructive breakdown and its mechanism on SiO2 films by TCE treatment. The result show that the breakdown current capacity increase with increasing the TCE flow-rate, treatment time and temperature, and reducing the oxygen partial pressure. However, excessive quantity of the TCE flow-rate and prolonging of treatment time make the breakdown characteristics degradation begin to appear. The results also indicate, the increment of breakdown current capacity is associate with the increment of density of electron trap in SiO2 films. In this paper, we propose a breakdown model of 'low barrier point-electrical field enhanced' which involve three processes of mutual reinforcement, and consider for the first time the effect of H2O in TCE oxidation on the breakdown characteristics. The restrained function of electron trap on electrical field enhanced in low barrier point is quoted, and analyze the mechanism for delay of destructive breakdown in TCE oxides.
The electron trapping at high-field and detrapping in thin thermally nitrided silicon oxide (SiOxNy) films are studied in the present work. It is observed that when the nitridation degree is the lighter, with the increasing of the nirridation time the effective electron trap surface concentration in the films increases rapidly, and the detrapping ratio of trapped electrons is almost zero and independent of the shorting time for samples and the strength (until 8MV/cm) and duration of application of external reverse field, and the depth of the electron trap level is the deeper; when the nitridation degree is the heavier with the further increasing of the nitridation time the effective electron trap surface concentration decreases and the depth of electron trap level becomes shallow gradually, and the detrapping ratio of trapped electrons gradually increases and is approximately dependent exponentially on the strength and duration of time application of external reverse field and is almost independent of the shorting time for the samples.
The electron trapping at high-field and detrapping in thin thermally nitrided silicon oxide (SiOxNy) films are studied in the present work. It is observed that when the nitridation degree is the lighter, with the increasing of the nirridation time the effective electron trap surface concentration in the films increases rapidly, and the detrapping ratio of trapped electrons is almost zero and independent of the shorting time for samples and the strength (until 8MV/cm) and duration of application of external reverse field, and the depth of the electron trap level is the deeper; when the nitridation degree is the heavier with the further increasing of the nitridation time the effective electron trap surface concentration decreases and the depth of electron trap level becomes shallow gradually, and the detrapping ratio of trapped electrons gradually increases and is approximately dependent exponentially on the strength and duration of time application of external reverse field and is almost independent of the shorting time for the samples.
Using Recursion method, we have studied the change of electronic structures caused by local substitution of Zn for Cu(2) in YBa2Cu3O7 material. It is found that the substitution has important effect on the properties of the substituted site and its neighbours, which include the partial wave densities of states, the type and strength of bonds, and the atomic valence of sites. On the basis of calculations, we analyze the mo ement of charge and believe that the decrease of hole concentration in CuO2 layers is the dominant factor in lowering the superconducting transition temperature of YBa2Cu3O7 when Zn substitutes Cu in small amounts.
Using Recursion method, we have studied the change of electronic structures caused by local substitution of Zn for Cu(2) in YBa2Cu3O7 material. It is found that the substitution has important effect on the properties of the substituted site and its neighbours, which include the partial wave densities of states, the type and strength of bonds, and the atomic valence of sites. On the basis of calculations, we analyze the mo ement of charge and believe that the decrease of hole concentration in CuO2 layers is the dominant factor in lowering the superconducting transition temperature of YBa2Cu3O7 when Zn substitutes Cu in small amounts.
In the samples of Sb proper doping Bi-Sr-Ca-Cu-O system, the content of the high temperature phase (110K phase) is obviously much higher than that of the Sb-free samples'. Sb has a function of accelerating the formation of the high Tc phase. For the nominal composition of Bi2-xSbxSr2Ca2.5Cu3.7Oy x = 0.1 is most beneficial to the formation of the high Tc phase, After quenching in liquid nitrogen and annealing at low teperatures, it is found that the low Tc phase (80K phase) is firstly formed when the samples are sintered at 865℃, then the low Tc phase changes to the high Tc phase, until all materials become the high Tc phase eventually. The value of Tc increases continuously with time lasting. If annealed at lower em-perature, the high Tc phase will change to the low Tc phase. Based on this discovering, after sintering at high temperature, for a long time, fast cooling to a low temperature, annealing for some time, then naturally cooling to room temperature, we have successfully prepared the high Tc single phase superconductor with zero resistance temperature 113K.
In the samples of Sb proper doping Bi-Sr-Ca-Cu-O system, the content of the high temperature phase (110K phase) is obviously much higher than that of the Sb-free samples'. Sb has a function of accelerating the formation of the high Tc phase. For the nominal composition of Bi2-xSbxSr2Ca2.5Cu3.7Oy x = 0.1 is most beneficial to the formation of the high Tc phase, After quenching in liquid nitrogen and annealing at low teperatures, it is found that the low Tc phase (80K phase) is firstly formed when the samples are sintered at 865℃, then the low Tc phase changes to the high Tc phase, until all materials become the high Tc phase eventually. The value of Tc increases continuously with time lasting. If annealed at lower em-perature, the high Tc phase will change to the low Tc phase. Based on this discovering, after sintering at high temperature, for a long time, fast cooling to a low temperature, annealing for some time, then naturally cooling to room temperature, we have successfully prepared the high Tc single phase superconductor with zero resistance temperature 113K.
The in-plane magnetic anisotropy constants of Fe40Ni40P12B8 and (Fe0.1CO0.5Ni0.4)78Si6B16 amorphous alloy ribbons in the as-quenched and annealed state have been measured with the torque magnetometer and the work of magnetization methods. The results show that the main part of the anisotropy constant measured by the torque magnetometer method for the as-quenched samples does not change after annealing and this part of anisotropy almost produces no influence on the magnetization curve.
The in-plane magnetic anisotropy constants of Fe40Ni40P12B8 and (Fe0.1CO0.5Ni0.4)78Si6B16 amorphous alloy ribbons in the as-quenched and annealed state have been measured with the torque magnetometer and the work of magnetization methods. The results show that the main part of the anisotropy constant measured by the torque magnetometer method for the as-quenched samples does not change after annealing and this part of anisotropy almost produces no influence on the magnetization curve.
Variation of S-parameter with the strain (S-ε curve) under different strain rate are investigated by combining Doppler broadening measurement with slow tensile test. Experimental results are as follows:1. Under slow strain rate, the S-ε curve in high purity iron does not tend to saturation. The slower the strain rate is, the more evident the 'non-saturation phenomenon'.2. Variations of S-ε curve with strain rate are attributed to the different configuration of dislocation distribution under different strain rates.3. As high purity iron is deformed, the increment of S-parameter depends not only on dislocation density but also on vacancy concentration, and we attibute the so called 'non-saturation phenomenon' of S-ε curve to the strain induced vacancies.
Variation of S-parameter with the strain (S-ε curve) under different strain rate are investigated by combining Doppler broadening measurement with slow tensile test. Experimental results are as follows:1. Under slow strain rate, the S-ε curve in high purity iron does not tend to saturation. The slower the strain rate is, the more evident the 'non-saturation phenomenon'.2. Variations of S-ε curve with strain rate are attributed to the different configuration of dislocation distribution under different strain rates.3. As high purity iron is deformed, the increment of S-parameter depends not only on dislocation density but also on vacancy concentration, and we attibute the so called 'non-saturation phenomenon' of S-ε curve to the strain induced vacancies.
The interaction between hydrogen atoms with defects in coldrolled nickel is investigated by Doppler broadening measurement. Experimental results show that the S-parameter in cold-rolled-hydrogen-charged nickel increases as compared with that of hydrogen-free cold-rolled nickel. And the increament of S-parameter depends on vacancy concentration, being almost independent of dislocation density. It is suggested that hydrogen atoms can act as centers of vacancy agglomeration, leading to the formation of vacancy cluster.
The interaction between hydrogen atoms with defects in coldrolled nickel is investigated by Doppler broadening measurement. Experimental results show that the S-parameter in cold-rolled-hydrogen-charged nickel increases as compared with that of hydrogen-free cold-rolled nickel. And the increament of S-parameter depends on vacancy concentration, being almost independent of dislocation density. It is suggested that hydrogen atoms can act as centers of vacancy agglomeration, leading to the formation of vacancy cluster.
Hel ultraviolet photoemission studies of CO coadsorption with different K coverages on W (100) surface show that the 1π/5σ level of α-CO shifts from 8.6eV to 9.3eV relative to the Fermi level while the K coverages increase, this indicates the increase of electron backdonation into 2π* of α-CO. Two independent peaks are found around 5.5 eV (Characteristic of β-Co), one is at 5.2eV, another is at 6.0eV. The peak at 5.2eV grows with increasing K coverages, its energy position is the same as that of O coadsorption with K on W(100) surface, this suggests that K forms bond to O of β-CO.
Hel ultraviolet photoemission studies of CO coadsorption with different K coverages on W (100) surface show that the 1π/5σ level of α-CO shifts from 8.6eV to 9.3eV relative to the Fermi level while the K coverages increase, this indicates the increase of electron backdonation into 2π* of α-CO. Two independent peaks are found around 5.5 eV (Characteristic of β-Co), one is at 5.2eV, another is at 6.0eV. The peak at 5.2eV grows with increasing K coverages, its energy position is the same as that of O coadsorption with K on W(100) surface, this suggests that K forms bond to O of β-CO.
A four valence cation conductor Sn4+ Montrnorillonite has been obtained in our lab. The valence state of migrating ion Sn4+ was confirmed with Mossbauer spectroscopy. Its electron eonductivity and AC conductivities were 5.1×10-7 and 1.5×10-4(S/cm) respectively. Some Sn/MnO2 batteries were made using this solid electrolyte with 1.2V OCV and 5mA short current for 13mm×3mm size.
A four valence cation conductor Sn4+ Montrnorillonite has been obtained in our lab. The valence state of migrating ion Sn4+ was confirmed with Mossbauer spectroscopy. Its electron eonductivity and AC conductivities were 5.1×10-7 and 1.5×10-4(S/cm) respectively. Some Sn/MnO2 batteries were made using this solid electrolyte with 1.2V OCV and 5mA short current for 13mm×3mm size.