Acta Physica Sinica - //m.suprmerch.com/ daily 15 2024-11-21 09:34:06 apsoffice@iphy.ac.cn apsoffice@iphy.ac.cn 2024-11-21 09:34:06 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[CRITICAL PHENOMENA IN OPTICAL BISTABILITY AND CHAOS]]> //m.suprmerch.com/en/article/doi/10.7498/aps.34.1233

The critical phenomena of bistability is discussed on the basis of the relaxation equation of the nonlinear systems with a time-delayed feedback. We find that the critical slowing down at the edges of bistable region possesses consistency with the divergence of the time duration of intermittency. The critica1 exponent is 1/2. We also find that, different from the critical points at the bistable region edges, there are consistencies with the period-doubling bifurcation points and split bifurcation points at the cusp point (in cusp catastrophe model of bistability). The critical exponent is 1. The abo-ve-mentioned results possess universal properties. The computer experiments have been made in the liquid crystal hybrid optical bistable device. The results are in agreement with the analyses.


Acta Physica Sinica. 1985 34(10): 1233-1240. Published 1985-05-05 ]]>

The critical phenomena of bistability is discussed on the basis of the relaxation equation of the nonlinear systems with a time-delayed feedback. We find that the critical slowing down at the edges of bistable region possesses consistency with the divergence of the time duration of intermittency. The critica1 exponent is 1/2. We also find that, different from the critical points at the bistable region edges, there are consistencies with the period-doubling bifurcation points and split bifurcation points at the cusp point (in cusp catastrophe model of bistability). The critical exponent is 1. The abo-ve-mentioned results possess universal properties. The computer experiments have been made in the liquid crystal hybrid optical bistable device. The results are in agreement with the analyses.


Acta Physica Sinica. 1985 34(10): 1233-1240. Published 1985-05-05 ]]>
1985-05-20T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 1985 34(10): 1233-1240. article doi:10.7498/aps.34.1233 10.7498/aps.34.1233 Acta Physica Sinica 34 10 1985-05-05 //m.suprmerch.com/en/article/doi/10.7498/aps.34.1233 1233-1240
<![CDATA[STUDY ON TRANSIENT OPTICAL BISTABILITY OF QUASI-RESONANT-ABSORPTIVE DYE MEDIUM]]> //m.suprmerch.com/en/article/doi/10.7498/aps.34.1241

Using intense pulsed laser beam of 5320 ? to excite the BDN dye solution inside the F-P interferometer, we have found the transient and intrinsic optical bistability effect. The various possible mechanisms to induce the refractive-index change of the sample medium and their relative contributions have been estimated; finally it is confirmed that in the duration of input laser pulse the refractive-index variation increases with time approximately in the form of semi-cubic parabola, and the main mechanism to cause this variation is the opto-thermal effect of the sample medium.


Acta Physica Sinica. 1985 34(10): 1241-1248. Published 1985-05-05 ]]>

Using intense pulsed laser beam of 5320 ? to excite the BDN dye solution inside the F-P interferometer, we have found the transient and intrinsic optical bistability effect. The various possible mechanisms to induce the refractive-index change of the sample medium and their relative contributions have been estimated; finally it is confirmed that in the duration of input laser pulse the refractive-index variation increases with time approximately in the form of semi-cubic parabola, and the main mechanism to cause this variation is the opto-thermal effect of the sample medium.


Acta Physica Sinica. 1985 34(10): 1241-1248. Published 1985-05-05 ]]>
1985-05-20T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 1985 34(10): 1241-1248. article doi:10.7498/aps.34.1241 10.7498/aps.34.1241 Acta Physica Sinica 34 10 1985-05-05 //m.suprmerch.com/en/article/doi/10.7498/aps.34.1241 1241-1248
<![CDATA[DETERMINATION OF THE RATIO OF THE SPIN ROTATION COUPLING CONSTANT TO THE SPIN EXCHANGE CONSTANT FOR THE K39Xe129VAN DER WAALS MOLECULE]]> //m.suprmerch.com/en/article/doi/10.7498/aps.34.1249

Optical pumping methods have been used to measure the ratio x of the spin rotation coupling constant to the spin exchange coupling constant of the K39Xe129Van der Waals molecule. The theory of these measuements is discussed in detail. The value x=γN/a= 4.8(1) is inferred from these studies.


Acta Physica Sinica. 1985 34(10): 1249-1260. Published 1985-05-05 ]]>

Optical pumping methods have been used to measure the ratio x of the spin rotation coupling constant to the spin exchange coupling constant of the K39Xe129Van der Waals molecule. The theory of these measuements is discussed in detail. The value x=γN/a= 4.8(1) is inferred from these studies.


Acta Physica Sinica. 1985 34(10): 1249-1260. Published 1985-05-05 ]]>
1985-05-20T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 1985 34(10): 1249-1260. article doi:10.7498/aps.34.1249 10.7498/aps.34.1249 Acta Physica Sinica 34 10 1985-05-05 //m.suprmerch.com/en/article/doi/10.7498/aps.34.1249 1249-1260
<![CDATA[VIBRATIONAL ENERGY TRANSFER STUDY OF DICHLOROMETHANE (CH2Cl2) BY LASER INDUCED FLUORESCENCE METHOD]]> //m.suprmerch.com/en/article/doi/10.7498/aps.34.1261

In this work, the vibrational energy transfer of organic molecule CH2C12 was studied with laser induced fluorescence method for the first time. The activation and deactiva-tion rate constants of modes ν3 and ν3/ν9 of pure CH2C12, as well as the effect of rare gases on the deactivation processes for ν3/ν9, were obtained. The relative propablities of energy transfer from ν3/ν9 vibrational modes of CH2Cl2 to translational degree of freedom were calculated by means of SSH theory for the collision relaxation processes of CH2Cl2-rare gas mixtures. A vibrational energy transfer channel in CH2C12 is also discussed.


Acta Physica Sinica. 1985 34(10): 1261-1269. Published 1985-05-05 ]]>

In this work, the vibrational energy transfer of organic molecule CH2C12 was studied with laser induced fluorescence method for the first time. The activation and deactiva-tion rate constants of modes ν3 and ν3/ν9 of pure CH2C12, as well as the effect of rare gases on the deactivation processes for ν3/ν9, were obtained. The relative propablities of energy transfer from ν3/ν9 vibrational modes of CH2Cl2 to translational degree of freedom were calculated by means of SSH theory for the collision relaxation processes of CH2Cl2-rare gas mixtures. A vibrational energy transfer channel in CH2C12 is also discussed.


Acta Physica Sinica. 1985 34(10): 1261-1269. Published 1985-05-05 ]]>
1985-05-20T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 1985 34(10): 1261-1269. article doi:10.7498/aps.34.1261 10.7498/aps.34.1261 Acta Physica Sinica 34 10 1985-05-05 //m.suprmerch.com/en/article/doi/10.7498/aps.34.1261 1261-1269
<![CDATA[INFRARED DIVERGENCE THEORY OF ULTRASONIC ABSORPTION IN GLASSES]]> //m.suprmerch.com/en/article/doi/10.7498/aps.34.1270

Starting from the unified theory of low-frequency fluctuation, dissipation, and relexation processes, we studied the ultrasonic absorption in the thermal activation pro-cess in glasses. The theory involves only a single relaxation time and differs from the theory of distributed relaxation times. Nontheless, it can explain the experimental cha-racteristics of the ultrasonic absorption in glasses and the universality of these charac-teristics independent of kinds of materials, which couldn't be interpreted by the pre-vious theory with the distribution of relaxation times.


Acta Physica Sinica. 1985 34(10): 1270-1279. Published 1985-05-05 ]]>

Starting from the unified theory of low-frequency fluctuation, dissipation, and relexation processes, we studied the ultrasonic absorption in the thermal activation pro-cess in glasses. The theory involves only a single relaxation time and differs from the theory of distributed relaxation times. Nontheless, it can explain the experimental cha-racteristics of the ultrasonic absorption in glasses and the universality of these charac-teristics independent of kinds of materials, which couldn't be interpreted by the pre-vious theory with the distribution of relaxation times.


Acta Physica Sinica. 1985 34(10): 1270-1279. Published 1985-05-05 ]]>
1985-05-20T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 1985 34(10): 1270-1279. article doi:10.7498/aps.34.1270 10.7498/aps.34.1270 Acta Physica Sinica 34 10 1985-05-05 //m.suprmerch.com/en/article/doi/10.7498/aps.34.1270 1270-1279
<![CDATA[THE TRIAL AND ERROR PROCEDURES IN THE DIRECT METHOD (Ⅰ)]]> //m.suprmerch.com/en/article/doi/10.7498/aps.34.1280

Some trial and error procedures are often used in the proccess of structure determination (calculating normalized structure factor, determining phase and builting molecular model) by the direct method. The present paper provides a procedure to calculate a trial molecular formula (TMF) on the basis of the diffraction data. Five unknown structures have been solved succesfully by means of the TMF. This method is helptul in extending the application of the direct method.


Acta Physica Sinica. 1985 34(10): 1280-1290. Published 1985-05-05 ]]>

Some trial and error procedures are often used in the proccess of structure determination (calculating normalized structure factor, determining phase and builting molecular model) by the direct method. The present paper provides a procedure to calculate a trial molecular formula (TMF) on the basis of the diffraction data. Five unknown structures have been solved succesfully by means of the TMF. This method is helptul in extending the application of the direct method.


Acta Physica Sinica. 1985 34(10): 1280-1290. Published 1985-05-05 ]]>
1985-05-20T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 1985 34(10): 1280-1290. article doi:10.7498/aps.34.1280 10.7498/aps.34.1280 Acta Physica Sinica 34 10 1985-05-05 //m.suprmerch.com/en/article/doi/10.7498/aps.34.1280 1280-1290
<![CDATA[A ASED-MO STUDY OF THE MICRO MECHANISM OF ACTIVATION OF CO ADSORBED ON Ni(100)AND POISONING BY THE SUBMONOLAYER S ATOM]]> //m.suprmerch.com/en/article/doi/10.7498/aps.34.1291

Using an atom superposition and electron delocalization molecular orbital (ASED-MO) theory, the micro-mechanism of activation of CO adsorbed on Ni(l00) and of poisoning by submonolayer S atom is studied. CO is found to bond to the top site more strongly than on the fourfold site. When CO is adsorbed on the top site, it will get 0.72 e on its antibonding 2π orbital, and its dissociation energy will reduce from 11.1 eV for free CO molecule to 2.15 eV. If CO is adsorbed on the fourfold site, the electrons on its 2π orbital will be 1.22 e and dissociation energy 1.85 eV. It seems likely that CO adsorbed on fourfold site is more active. Our binding energy calculations have verified that one S atom adsorbed on Ni(l00) will inhibit 4 nearest top sites and 4 nearest fourfold sites from adsorbing CO molecule, but will not give any important affection on farther sites. These results support the idea that the dominant effect of adsorbed S atom is 'structural effect'. These 'blockage' effect by the adsorbed S atom, i.e. the reduction of the active sites, and some other factors, result in the poisoning of Ni sur-faces by submonolayer S atom.


Acta Physica Sinica. 1985 34(10): 1291-1298. Published 1985-05-05 ]]>

Using an atom superposition and electron delocalization molecular orbital (ASED-MO) theory, the micro-mechanism of activation of CO adsorbed on Ni(l00) and of poisoning by submonolayer S atom is studied. CO is found to bond to the top site more strongly than on the fourfold site. When CO is adsorbed on the top site, it will get 0.72 e on its antibonding 2π orbital, and its dissociation energy will reduce from 11.1 eV for free CO molecule to 2.15 eV. If CO is adsorbed on the fourfold site, the electrons on its 2π orbital will be 1.22 e and dissociation energy 1.85 eV. It seems likely that CO adsorbed on fourfold site is more active. Our binding energy calculations have verified that one S atom adsorbed on Ni(l00) will inhibit 4 nearest top sites and 4 nearest fourfold sites from adsorbing CO molecule, but will not give any important affection on farther sites. These results support the idea that the dominant effect of adsorbed S atom is 'structural effect'. These 'blockage' effect by the adsorbed S atom, i.e. the reduction of the active sites, and some other factors, result in the poisoning of Ni sur-faces by submonolayer S atom.


Acta Physica Sinica. 1985 34(10): 1291-1298. Published 1985-05-05 ]]>
1985-05-20T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 1985 34(10): 1291-1298. article doi:10.7498/aps.34.1291 10.7498/aps.34.1291 Acta Physica Sinica 34 10 1985-05-05 //m.suprmerch.com/en/article/doi/10.7498/aps.34.1291 1291-1298
<![CDATA[INVESTIGATION OF CO AND NO CHEMISORPTION ON THE Ⅷ GROUP TRANSITION METAL SURFACE BY Xα-DV METHOD(Ⅰ)——ELECTRONIC STRUCTURE OF CHEMISOPTION OF CO ON Rh(111) SURFACE]]> //m.suprmerch.com/en/article/doi/10.7498/aps.34.1299

In this paper, the electronic structure of chemisorption of CO on Rh(lll) surface (θ≤l/3) has been calculated by the method of the self-consistent Hartree-Fock-Slater molecular cluster. The variation of the energy levels and total energy with respect to the vertical distance of the CO molecule above this surface is obtained. The optimized bond distance determined from the total energy curve is 1.85 ?, which is quite close to experimental result 1.95±0.1?. The binding energy is 0.98 eV, which is smaller than the experimental adsorption energy of 1.3 eV. The total density of states with above bond distance is calculated and it is in good agreement with the UPS result considering final state and relaxation effect. The bonding and antibonding character for the CO valence level have also been studied by analysis of the variations of the molecular eigenvalues when the CO molecule approaches the surface. The charge transfer for CO chemisorption on transition metal Rh is investigated through a Milliken population analysis and the analysis of coefficients of cluster wavefunction which is expanded by using CO molecular wavefunction. This charge transfer causes the activation of absorbed CO molecules.


Acta Physica Sinica. 1985 34(10): 1299-1305. Published 1985-05-05 ]]>

In this paper, the electronic structure of chemisorption of CO on Rh(lll) surface (θ≤l/3) has been calculated by the method of the self-consistent Hartree-Fock-Slater molecular cluster. The variation of the energy levels and total energy with respect to the vertical distance of the CO molecule above this surface is obtained. The optimized bond distance determined from the total energy curve is 1.85 ?, which is quite close to experimental result 1.95±0.1?. The binding energy is 0.98 eV, which is smaller than the experimental adsorption energy of 1.3 eV. The total density of states with above bond distance is calculated and it is in good agreement with the UPS result considering final state and relaxation effect. The bonding and antibonding character for the CO valence level have also been studied by analysis of the variations of the molecular eigenvalues when the CO molecule approaches the surface. The charge transfer for CO chemisorption on transition metal Rh is investigated through a Milliken population analysis and the analysis of coefficients of cluster wavefunction which is expanded by using CO molecular wavefunction. This charge transfer causes the activation of absorbed CO molecules.


Acta Physica Sinica. 1985 34(10): 1299-1305. Published 1985-05-05 ]]>
1985-05-20T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 1985 34(10): 1299-1305. article doi:10.7498/aps.34.1299 10.7498/aps.34.1299 Acta Physica Sinica 34 10 1985-05-05 //m.suprmerch.com/en/article/doi/10.7498/aps.34.1299 1299-1305
<![CDATA[INVESTIGATION OF CO AND NO CHEMISORPTION ON THE Ⅷ GROUP TRANSITION METAL SURFACE BY Xα-DV METHOD(Ⅱ)——CHEMISORPTION OP NO ON PD(111) SURFACE]]> //m.suprmerch.com/en/article/doi/10.7498/aps.34.1306

The Chemisorption of NO on Pd (111) surface is calculated using Xα-DV method. It's electronic structure, including spectrum of the ground state valence levels, density of states, and the charge transfer between adsorbate and substrate, is obtained. The interaction between adsorbed NO molecules is included in our calculations. The results of DOS are in good agreement with UPS, supporting the LEBD structural analysis, and the adsorption height is determined to be 1.27 ?. Our theoretical results have verified that the interaction between NO is rather important in the chemisorption of NO on Pd surfaces. The activation of adsorbed NO on Pd(lll) is discussed. It is evident from our results that the charge transfer between adsorbed NO and substrate is similar to CO adsorption on transition metal. Finally, we found that the adsorption of NO does not significantly affect the valence band of Pd.


Acta Physica Sinica. 1985 34(10): 1306-1314. Published 1985-05-05 ]]>

The Chemisorption of NO on Pd (111) surface is calculated using Xα-DV method. It's electronic structure, including spectrum of the ground state valence levels, density of states, and the charge transfer between adsorbate and substrate, is obtained. The interaction between adsorbed NO molecules is included in our calculations. The results of DOS are in good agreement with UPS, supporting the LEBD structural analysis, and the adsorption height is determined to be 1.27 ?. Our theoretical results have verified that the interaction between NO is rather important in the chemisorption of NO on Pd surfaces. The activation of adsorbed NO on Pd(lll) is discussed. It is evident from our results that the charge transfer between adsorbed NO and substrate is similar to CO adsorption on transition metal. Finally, we found that the adsorption of NO does not significantly affect the valence band of Pd.


Acta Physica Sinica. 1985 34(10): 1306-1314. Published 1985-05-05 ]]>
1985-05-20T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 1985 34(10): 1306-1314. article doi:10.7498/aps.34.1306 10.7498/aps.34.1306 Acta Physica Sinica 34 10 1985-05-05 //m.suprmerch.com/en/article/doi/10.7498/aps.34.1306 1306-1314
<![CDATA[EXPERIMENTAL DETERMINATION OF THE STEREOCHIMI-CAL STRUCTURE OF H3+]]> //m.suprmerch.com/en/article/doi/10.7498/aps.34.1315

The measurement 011 the sterochimical structure of H3+ molecular ion is reported. It makes use of the Coulomb explosion of a fast molecular ion. It is shown that the structure is equilaterally triangular in shape. The mean value of most probable inter-proton separations is found to be 0.98±0.03?. A set of high resolution experimental arrangment of ours is also described.


Acta Physica Sinica. 1985 34(10): 1315-1321. Published 1985-05-05 ]]>

The measurement 011 the sterochimical structure of H3+ molecular ion is reported. It makes use of the Coulomb explosion of a fast molecular ion. It is shown that the structure is equilaterally triangular in shape. The mean value of most probable inter-proton separations is found to be 0.98±0.03?. A set of high resolution experimental arrangment of ours is also described.


Acta Physica Sinica. 1985 34(10): 1315-1321. Published 1985-05-05 ]]>
1985-05-20T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 1985 34(10): 1315-1321. article doi:10.7498/aps.34.1315 10.7498/aps.34.1315 Acta Physica Sinica 34 10 1985-05-05 //m.suprmerch.com/en/article/doi/10.7498/aps.34.1315 1315-1321
<![CDATA[PRESSURE EFFECT ON THE STABILITY AND PHASE TRANSFORMATION OF THE ε-PHASE IN SPLAT QUENCHING Fe-C-Sb ALLOY]]> //m.suprmerch.com/en/article/doi/10.7498/aps.34.1322

Pressure effect on the phase transformation process of the ε-phase of splat quenching Pe-C-Sb alloy has been investigated by using X-ray powder photography. The experimental results show that high pressure will not only increase the stability of the ε-phase remarkably but also change its phase transformation process. At 4.7 GPa, as the temperature of stability of ε-phase increases to 450℃, a new metastable phase of orthorhombic structure, being absent at normal pressure, will appear. By raising annealing temperature to 560℃, the orthorhombic metastable phase begins to transform into Fe3C which will decompose into carbon (graphite) and γ-Fe on further increasing annealing temperature to 800℃. At this time, the alloy is composed of C (graphite), γ-Fe, Sb and another unknown phase.


Acta Physica Sinica. 1985 34(10): 1322-1326. Published 1985-05-05 ]]>

Pressure effect on the phase transformation process of the ε-phase of splat quenching Pe-C-Sb alloy has been investigated by using X-ray powder photography. The experimental results show that high pressure will not only increase the stability of the ε-phase remarkably but also change its phase transformation process. At 4.7 GPa, as the temperature of stability of ε-phase increases to 450℃, a new metastable phase of orthorhombic structure, being absent at normal pressure, will appear. By raising annealing temperature to 560℃, the orthorhombic metastable phase begins to transform into Fe3C which will decompose into carbon (graphite) and γ-Fe on further increasing annealing temperature to 800℃. At this time, the alloy is composed of C (graphite), γ-Fe, Sb and another unknown phase.


Acta Physica Sinica. 1985 34(10): 1322-1326. Published 1985-05-05 ]]>
1985-05-20T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 1985 34(10): 1322-1326. article doi:10.7498/aps.34.1322 10.7498/aps.34.1322 Acta Physica Sinica 34 10 1985-05-05 //m.suprmerch.com/en/article/doi/10.7498/aps.34.1322 1322-1326
<![CDATA[THE CRYSTALLIZATION PROCESS OF METGLASS (Fe0.1Co0.55Ni0.35)78Si8B14 AND THE EFFECT OF HIGH PRESSURE (Ⅱ)——The Crystallization Temperature and The Crystallization Activation Energy]]> //m.suprmerch.com/en/article/doi/10.7498/aps.34.1327

In this paper, the pressure dependence of the crystallization temperature Tx and the crystallization activation energy △EX of metglass (Fe0.1Co0.55Ni0.35)78Si8B14 werestudied by measuring the electrical resistivity in-situ under pressure up to 3 GPas. It was found that application of high pressure not linearly, even not monotonicaly riases the Tx, as usually described in literatures for pressure dependence of Tx in metglasses, but shows some local detours on Tx vs. P curve in a general rising tendency. △Ex shows same behaviour analogous to that of Tx as the pressure rises. An analytical discussion indicates that pressure promotes the nucleation process and restrains the diffusional growing up of the crystallized nuclei on heating the metglass. As a combined result of the mutual contrary effects of pressure on nucleation activation energy a,nd diffusion activation energy, it gives rise the above non-monotonic rising behaviour of △Ex and Tx of the metglass studied. In addition to △Ex, pressure may also markedly affect the preexponential factor and produces a considerable change on crystallization temperature.


Acta Physica Sinica. 1985 34(10): 1327-1335. Published 1985-05-05 ]]>

In this paper, the pressure dependence of the crystallization temperature Tx and the crystallization activation energy △EX of metglass (Fe0.1Co0.55Ni0.35)78Si8B14 werestudied by measuring the electrical resistivity in-situ under pressure up to 3 GPas. It was found that application of high pressure not linearly, even not monotonicaly riases the Tx, as usually described in literatures for pressure dependence of Tx in metglasses, but shows some local detours on Tx vs. P curve in a general rising tendency. △Ex shows same behaviour analogous to that of Tx as the pressure rises. An analytical discussion indicates that pressure promotes the nucleation process and restrains the diffusional growing up of the crystallized nuclei on heating the metglass. As a combined result of the mutual contrary effects of pressure on nucleation activation energy a,nd diffusion activation energy, it gives rise the above non-monotonic rising behaviour of △Ex and Tx of the metglass studied. In addition to △Ex, pressure may also markedly affect the preexponential factor and produces a considerable change on crystallization temperature.


Acta Physica Sinica. 1985 34(10): 1327-1335. Published 1985-05-05 ]]>
1985-05-20T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 1985 34(10): 1327-1335. article doi:10.7498/aps.34.1327 10.7498/aps.34.1327 Acta Physica Sinica 34 10 1985-05-05 //m.suprmerch.com/en/article/doi/10.7498/aps.34.1327 1327-1335
<![CDATA[STUDIES ON THE STRUCTURE OF AMORPHOUS MoS3 AS CATHODE MATERIALS IN LITHIUM BATTERIES]]> //m.suprmerch.com/en/article/doi/10.7498/aps.34.1336

The structure of amorphous MoS3 as the cathode materials in lithium batteries was studied by using X-ray diffraction method and X-ray photoelectron spectroscopy. The results revealed that the structure of amorphous MoS3 is built by homogeneously eandomly stacking of the MoS2 basic unit S-Mo-S sand wich layvs and the amorphous sulphus chains Sn.


Acta Physica Sinica. 1985 34(10): 1336-1341. Published 1985-05-05 ]]>

The structure of amorphous MoS3 as the cathode materials in lithium batteries was studied by using X-ray diffraction method and X-ray photoelectron spectroscopy. The results revealed that the structure of amorphous MoS3 is built by homogeneously eandomly stacking of the MoS2 basic unit S-Mo-S sand wich layvs and the amorphous sulphus chains Sn.


Acta Physica Sinica. 1985 34(10): 1336-1341. Published 1985-05-05 ]]>
1985-05-20T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 1985 34(10): 1336-1341. article doi:10.7498/aps.34.1336 10.7498/aps.34.1336 Acta Physica Sinica 34 10 1985-05-05 //m.suprmerch.com/en/article/doi/10.7498/aps.34.1336 1336-1341
<![CDATA[A(4 + 1)-DIMENSIONAL COSMOLOGICAL MODEL]]> //m.suprmerch.com/en/article/doi/10.7498/aps.34.1342

The (4+1)-dimensional cosmological model discussed in this paper is a direct product of the usual 4-dimensional spacetime and a. 1-dimensional compaetified internal space. The energy density of the 4-dimensional spacetime is supposed to be dominated by incoherent radiation and the energy-momentum tensor of the internal subspace is a step function. By solving the 5-dimensional Einstein field equations without cosmolog-ical term we get the de-Sitter solution to describe the usual spacetime and at a certain time it changes to the radiation-dominated solution for standard model, and the size of the internal subspace changes with time in a form of oscillation with amplitude attenuating and then contracts to a constant.


Acta Physica Sinica. 1985 34(10): 1342-1347. Published 1985-05-05 ]]>

The (4+1)-dimensional cosmological model discussed in this paper is a direct product of the usual 4-dimensional spacetime and a. 1-dimensional compaetified internal space. The energy density of the 4-dimensional spacetime is supposed to be dominated by incoherent radiation and the energy-momentum tensor of the internal subspace is a step function. By solving the 5-dimensional Einstein field equations without cosmolog-ical term we get the de-Sitter solution to describe the usual spacetime and at a certain time it changes to the radiation-dominated solution for standard model, and the size of the internal subspace changes with time in a form of oscillation with amplitude attenuating and then contracts to a constant.


Acta Physica Sinica. 1985 34(10): 1342-1347. Published 1985-05-05 ]]>
1985-05-20T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 1985 34(10): 1342-1347. article doi:10.7498/aps.34.1342 10.7498/aps.34.1342 Acta Physica Sinica 34 10 1985-05-05 //m.suprmerch.com/en/article/doi/10.7498/aps.34.1342 1342-1347
<![CDATA[EXPERIMENTAL INVESTIGATION OF INSTABILITY AND CHAOS ON THREE MODE He-Ne(6328?) LASER]]> //m.suprmerch.com/en/article/doi/10.7498/aps.34.1348

Instability and chaos in a three-mode He-Ne (6328?) laser was studied by varying discharge current and cavity length. Period doubling, two-frequency and intermit-tency routes to chaos have been observed.


Acta Physica Sinica. 1985 34(10): 1348-1353. Published 1985-05-05 ]]>

Instability and chaos in a three-mode He-Ne (6328?) laser was studied by varying discharge current and cavity length. Period doubling, two-frequency and intermit-tency routes to chaos have been observed.


Acta Physica Sinica. 1985 34(10): 1348-1353. Published 1985-05-05 ]]>
1985-05-20T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 1985 34(10): 1348-1353. article doi:10.7498/aps.34.1348 10.7498/aps.34.1348 Acta Physica Sinica 34 10 1985-05-05 //m.suprmerch.com/en/article/doi/10.7498/aps.34.1348 1348-1353
<![CDATA[PYROELECTRIC PROPERTIES OF METHYL P-HYDROXYBENZOATE CRYSTALS (P-MHB)]]> //m.suprmerch.com/en/article/doi/10.7498/aps.34.1354

The methyl P-hydroxybenzoats cryslal is a organic pyroelectric crystal. A thorough experimental study has been carried out on its pyroelectric effect, electric condutance, hysteresis loop and other relevant properties.


Acta Physica Sinica. 1985 34(10): 1354-1358. Published 1985-05-05 ]]>

The methyl P-hydroxybenzoats cryslal is a organic pyroelectric crystal. A thorough experimental study has been carried out on its pyroelectric effect, electric condutance, hysteresis loop and other relevant properties.


Acta Physica Sinica. 1985 34(10): 1354-1358. Published 1985-05-05 ]]>
1985-05-20T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 1985 34(10): 1354-1358. article doi:10.7498/aps.34.1354 10.7498/aps.34.1354 Acta Physica Sinica 34 10 1985-05-05 //m.suprmerch.com/en/article/doi/10.7498/aps.34.1354 1354-1358
<![CDATA[THE INTERACTION PICTURE IN THE CLOSED TIME PATH GREEN'S FUNCTIONS]]> //m.suprmerch.com/en/article/doi/10.7498/aps.34.1359

It is clarified that the interaction picture introduced in CTPGF ought to be the incoming one and the perturbation expansion of CTPGF to be developed also in this sense.


Acta Physica Sinica. 1985 34(10): 1359-1362. Published 1985-05-05 ]]>

It is clarified that the interaction picture introduced in CTPGF ought to be the incoming one and the perturbation expansion of CTPGF to be developed also in this sense.


Acta Physica Sinica. 1985 34(10): 1359-1362. Published 1985-05-05 ]]>
1985-05-20T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 1985 34(10): 1359-1362. article doi:10.7498/aps.34.1359 10.7498/aps.34.1359 Acta Physica Sinica 34 10 1985-05-05 //m.suprmerch.com/en/article/doi/10.7498/aps.34.1359 1359-1362
<![CDATA[XPS AND AES STUDY OF AlxGa1-xP SOLID SOLUTIONS]]> //m.suprmerch.com/en/article/doi/10.7498/aps.34.1363

The solid solution AlxGa1-xP(0≤x≤0.64) has been investigated by XPS and ABS.The experimental results show that the binding energy of P21, core level decreases and the top of the valence band recedes with increasing Al-content. Moreover the weak Auger peaks of GaP have been identified and clarified.


Acta Physica Sinica. 1985 34(10): 1363-1367. Published 1985-05-05 ]]>

The solid solution AlxGa1-xP(0≤x≤0.64) has been investigated by XPS and ABS.The experimental results show that the binding energy of P21, core level decreases and the top of the valence band recedes with increasing Al-content. Moreover the weak Auger peaks of GaP have been identified and clarified.


Acta Physica Sinica. 1985 34(10): 1363-1367. Published 1985-05-05 ]]>
1985-05-20T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 1985 34(10): 1363-1367. article doi:10.7498/aps.34.1363 10.7498/aps.34.1363 Acta Physica Sinica 34 10 1985-05-05 //m.suprmerch.com/en/article/doi/10.7498/aps.34.1363 1363-1367
<![CDATA[THE INHOMOGENEOUS STATES OF SUPERCONDUCTING TIN FILMS UNDER PHONON INJECTION]]> //m.suprmerch.com/en/article/doi/10.7498/aps.34.1368

Using Sn-I-Sn-I-Sn-I-Sn triple tunnel junctions, some spatial inhomogeneous states in superconducting tin films were observed under strong phonon injection.


Acta Physica Sinica. 1985 34(10): 1368-1372. Published 1985-05-05 ]]>

Using Sn-I-Sn-I-Sn-I-Sn triple tunnel junctions, some spatial inhomogeneous states in superconducting tin films were observed under strong phonon injection.


Acta Physica Sinica. 1985 34(10): 1368-1372. Published 1985-05-05 ]]>
1985-05-20T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 1985 34(10): 1368-1372. article doi:10.7498/aps.34.1368 10.7498/aps.34.1368 Acta Physica Sinica 34 10 1985-05-05 //m.suprmerch.com/en/article/doi/10.7498/aps.34.1368 1368-1372
<![CDATA[IS VPd3 A WEAK ITINERANT FERROMAGNET?]]> //m.suprmerch.com/en/article/doi/10.7498/aps.34.1373

The electronic structure and the X-ray photoemission spectrum for VPd3 were calculated using the self-consistent LMTO method. The general feature and the peak positions of the density of states were in reasonable agreement with Williams et al. Contrary to their result μs~1.4μB for VPd3, the calculated Stoner parameter for VPd3 is 1.04, which indicated that VPd3 may be considered as one of the weak itinerant magnets likely. Nevertheless, a discrepancy between ours and Burmester et al., who found no evidence for magnetic ordering in VPd3 down to 1.6 K, remained to be solved.


Acta Physica Sinica. 1985 34(10): 1373-1376. Published 1985-05-05 ]]>

The electronic structure and the X-ray photoemission spectrum for VPd3 were calculated using the self-consistent LMTO method. The general feature and the peak positions of the density of states were in reasonable agreement with Williams et al. Contrary to their result μs~1.4μB for VPd3, the calculated Stoner parameter for VPd3 is 1.04, which indicated that VPd3 may be considered as one of the weak itinerant magnets likely. Nevertheless, a discrepancy between ours and Burmester et al., who found no evidence for magnetic ordering in VPd3 down to 1.6 K, remained to be solved.


Acta Physica Sinica. 1985 34(10): 1373-1376. Published 1985-05-05 ]]>
1985-05-20T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 1985 34(10): 1373-1376. article doi:10.7498/aps.34.1373 10.7498/aps.34.1373 Acta Physica Sinica 34 10 1985-05-05 //m.suprmerch.com/en/article/doi/10.7498/aps.34.1373 1373-1376