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//www.getgobooth.com/en/article/doi/10.7498/aps.30.145
Author(s): QIAN ZU-WEN <br/><p>In this paper, it has been shown that in the near field of parametric sound array, the Fresnel's approximation proposed by Berktay is inappropriate.</p> <br/>Acta Physica Sinica. 1981 30(11): 145-147. Published 2005-07-27
Author(s): QIAN ZU-WEN <br/><p>In this paper, it has been shown that in the near field of parametric sound array, the Fresnel's approximation proposed by Berktay is inappropriate.</p> <br/>Acta Physica Sinica. 1981 30(11): 145-147. Published 2005-07-27
ON THE NEAR FIELD OF PARAMETRIC SOUND ARRAY
QIAN ZU-WEN
2005-07-27
Personal use only, all commercial or other reuse prohibited
Acta Physica Sinica. 1981 30(11): 145-147.
article
doi:10.7498/aps.30.145
10.7498/aps.30.145
Acta Physica Sinica
30
11
2005-07-27
//www.getgobooth.com/en/article/doi/10.7498/aps.30.145
145-147
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//www.getgobooth.com/en/article/doi/10.7498/aps.30.148
Author(s): AN YING, CHEN SHI, GUO HAN-YING <br/><p>A U1-bundle formalism for the Born-Infeld electrodynamics is proposed and the equation of motion for a test particle in the Born-Infeld electromagnetic field is given. There are two forces acting on the test particle, one corresponds to the Lorentz force and the other the Poincaré stress.</p> <br/>Acta Physica Sinica. 1981 30(11): 148-150. Published 2005-07-27
Author(s): AN YING, CHEN SHI, GUO HAN-YING <br/><p>A U1-bundle formalism for the Born-Infeld electrodynamics is proposed and the equation of motion for a test particle in the Born-Infeld electromagnetic field is given. There are two forces acting on the test particle, one corresponds to the Lorentz force and the other the Poincaré stress.</p> <br/>Acta Physica Sinica. 1981 30(11): 148-150. Published 2005-07-27
A U1 PRINCIPAL BUNDLE THEORY FOR THE BORN-INFELD ELECTRODYNAMICS
AN YING, CHEN SHI, GUO HAN-YING
2005-07-27
Personal use only, all commercial or other reuse prohibited
Acta Physica Sinica. 1981 30(11): 148-150.
article
doi:10.7498/aps.30.148
10.7498/aps.30.148
Acta Physica Sinica
30
11
2005-07-27
//www.getgobooth.com/en/article/doi/10.7498/aps.30.148
148-150
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//www.getgobooth.com/en/article/doi/10.7498/aps.30.151
Author(s): ZHANG YANG-ZHONG <br/><p>By using the perturbative expansions of 〈j⊥· E⊥〉 it was proved that the coherent renormalization theory acquired the energy conservation of non-linear drift waves within the sixth order.</p> <br/>Acta Physica Sinica. 1981 30(11): 151-154. Published 2005-07-27
Author(s): ZHANG YANG-ZHONG <br/><p>By using the perturbative expansions of 〈j⊥· E⊥〉 it was proved that the coherent renormalization theory acquired the energy conservation of non-linear drift waves within the sixth order.</p> <br/>Acta Physica Sinica. 1981 30(11): 151-154. Published 2005-07-27
ENERGY CONSERVATION OF NON-LINEAR DRIFT WAVES IN THE COHERENT RENORMALIZATION
ZHANG YANG-ZHONG
2005-07-27
Personal use only, all commercial or other reuse prohibited
Acta Physica Sinica. 1981 30(11): 151-154.
article
doi:10.7498/aps.30.151
10.7498/aps.30.151
Acta Physica Sinica
30
11
2005-07-27
//www.getgobooth.com/en/article/doi/10.7498/aps.30.151
151-154
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//www.getgobooth.com/en/article/doi/10.7498/aps.30.1415
Author(s): HE XIAN-TU <br/><p>It is well known that, in the bremsstrahlung formula derived by Birmingham and Dawson, the screening effects of ions on the fields were discarded. It is unapt to do so. In this paper a corrected formula, including the polarization effects of ionic fields, is derived. In many cases, the screening effects of ions can considerably reduce the energy of the bremsstrahlung.</p> <br/>Acta Physica Sinica. 1981 30(11): 1415-1422. Published 2005-07-29
Author(s): HE XIAN-TU <br/><p>It is well known that, in the bremsstrahlung formula derived by Birmingham and Dawson, the screening effects of ions on the fields were discarded. It is unapt to do so. In this paper a corrected formula, including the polarization effects of ionic fields, is derived. In many cases, the screening effects of ions can considerably reduce the energy of the bremsstrahlung.</p> <br/>Acta Physica Sinica. 1981 30(11): 1415-1422. Published 2005-07-29
THE COLLECTIVE EFFECTS ON THE BREMSSTRAHLUNG IN PLASMA
HE XIAN-TU
2005-07-29
Personal use only, all commercial or other reuse prohibited
Acta Physica Sinica. 1981 30(11): 1415-1422.
article
doi:10.7498/aps.30.1415
10.7498/aps.30.1415
Acta Physica Sinica
30
11
2005-07-29
//www.getgobooth.com/en/article/doi/10.7498/aps.30.1415
1415-1422
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//www.getgobooth.com/en/article/doi/10.7498/aps.30.1423
Author(s): TAN WEI-HEN, WANG RUN-WEN, DING LI-MING <br/><p>On the basis of Vlasov equation, we extend the results of our previous work [10] and obtain the general coupling equations for the electrons, ions of plasmas and the electromagnetic radiation. We have solved these coupling equations, and obtaind the threshold powers and growth rates of the stimulated scattering and harmonic radiation. Finally, we propose a successive generating mechanism of the harmanics and sub-harmonics, such a mechanism is in agreement with the experimental results in the literatures.</p> <br/>Acta Physica Sinica. 1981 30(11): 1423-1437. Published 2005-07-29
Author(s): TAN WEI-HEN, WANG RUN-WEN, DING LI-MING <br/><p>On the basis of Vlasov equation, we extend the results of our previous work [10] and obtain the general coupling equations for the electrons, ions of plasmas and the electromagnetic radiation. We have solved these coupling equations, and obtaind the threshold powers and growth rates of the stimulated scattering and harmonic radiation. Finally, we propose a successive generating mechanism of the harmanics and sub-harmonics, such a mechanism is in agreement with the experimental results in the literatures.</p> <br/>Acta Physica Sinica. 1981 30(11): 1423-1437. Published 2005-07-29
STIMULATED SCATTERING AND HARMONIC RADIATION OF HOMOGENEOUS AND INHOMOGENEOUS LASER PLASMAS
TAN WEI-HEN, WANG RUN-WEN, DING LI-MING
2005-07-29
Personal use only, all commercial or other reuse prohibited
Acta Physica Sinica. 1981 30(11): 1423-1437.
article
doi:10.7498/aps.30.1423
10.7498/aps.30.1423
Acta Physica Sinica
30
11
2005-07-29
//www.getgobooth.com/en/article/doi/10.7498/aps.30.1423
1423-1437
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//www.getgobooth.com/en/article/doi/10.7498/aps.30.1438
Author(s): KE FU-JIU, CHEN YIAN-PING, ZHOU YU-MEI, C. S. WU <br/><p>We consider the nonlinear saturation of a fast x mode instability near the electron cyclotron frequency due to electron population inversion. A quasilinear theory is discussed. The corresponding saturation time, amplitudes as well as the temporal evolution of the electron distribution functions are also studied.</p> <br/>Acta Physica Sinica. 1981 30(11): 1438-1447. Published 2005-07-29
Author(s): KE FU-JIU, CHEN YIAN-PING, ZHOU YU-MEI, C. S. WU <br/><p>We consider the nonlinear saturation of a fast x mode instability near the electron cyclotron frequency due to electron population inversion. A quasilinear theory is discussed. The corresponding saturation time, amplitudes as well as the temporal evolution of the electron distribution functions are also studied.</p> <br/>Acta Physica Sinica. 1981 30(11): 1438-1447. Published 2005-07-29
THE QAUSILINEAR THEORY OF AN ELECTROMAGNETIC CYCLOTRON INSTABILITY
KE FU-JIU, CHEN YIAN-PING, ZHOU YU-MEI, C. S. WU
2005-07-29
Personal use only, all commercial or other reuse prohibited
Acta Physica Sinica. 1981 30(11): 1438-1447.
article
doi:10.7498/aps.30.1438
10.7498/aps.30.1438
Acta Physica Sinica
30
11
2005-07-29
//www.getgobooth.com/en/article/doi/10.7498/aps.30.1438
1438-1447
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//www.getgobooth.com/en/article/doi/10.7498/aps.30.1448
Author(s): CHEN LIU, ZHOU YU-MEI, CAI SHI-DONG <br/><p>Under a quite general condition, we show that a very strong high frequency pump can only excite the OTSI-like absolute instabilities in either uniform or nonuniform plasmas.Such property can be extended to magnetized plasmas as well.</p> <br/>Acta Physica Sinica. 1981 30(11): 1448-1455. Published 2005-07-29
Author(s): CHEN LIU, ZHOU YU-MEI, CAI SHI-DONG <br/><p>Under a quite general condition, we show that a very strong high frequency pump can only excite the OTSI-like absolute instabilities in either uniform or nonuniform plasmas.Such property can be extended to magnetized plasmas as well.</p> <br/>Acta Physica Sinica. 1981 30(11): 1448-1455. Published 2005-07-29
THE CHARACTERISTIC OF PARAMETRIC INSTABILITIES EXCITED BY HIGH FREQUENCY PUMPS
CHEN LIU, ZHOU YU-MEI, CAI SHI-DONG
2005-07-29
Personal use only, all commercial or other reuse prohibited
Acta Physica Sinica. 1981 30(11): 1448-1455.
article
doi:10.7498/aps.30.1448
10.7498/aps.30.1448
Acta Physica Sinica
30
11
2005-07-29
//www.getgobooth.com/en/article/doi/10.7498/aps.30.1448
1448-1455
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//www.getgobooth.com/en/article/doi/10.7498/aps.30.1456
Author(s): XU JI-REN, HUANG NAN-TANG, JIANG YI-FENG, FU GUANG-SHENG, WU ZHEN-QIU <br/><p>The absorption spectrum of the vibrational excited state in BC13 has been obtained by means of a infrared double resonance technique. A variety of relaxation processes and energy transfer processes were observed. The relationship PτV-V(11BCl3)= 3μs·torr has been obtained. A radial sound modulation was observed on the double resonance signal. The sound velocity is 2×104cm/sec and it agrees with the calculated value.</p> <br/>Acta Physica Sinica. 1981 30(11): 1456-1463. Published 2005-07-29
Author(s): XU JI-REN, HUANG NAN-TANG, JIANG YI-FENG, FU GUANG-SHENG, WU ZHEN-QIU <br/><p>The absorption spectrum of the vibrational excited state in BC13 has been obtained by means of a infrared double resonance technique. A variety of relaxation processes and energy transfer processes were observed. The relationship PτV-V(11BCl3)= 3μs·torr has been obtained. A radial sound modulation was observed on the double resonance signal. The sound velocity is 2×104cm/sec and it agrees with the calculated value.</p> <br/>Acta Physica Sinica. 1981 30(11): 1456-1463. Published 2005-07-29
INFRARED ABSORPTION INVESTIGATION OF VIBRATIONAL EXCITED RELAXATIONS IN BCl3
XU JI-REN, HUANG NAN-TANG, JIANG YI-FENG, FU GUANG-SHENG, WU ZHEN-QIU
2005-07-29
Personal use only, all commercial or other reuse prohibited
Acta Physica Sinica. 1981 30(11): 1456-1463.
article
doi:10.7498/aps.30.1456
10.7498/aps.30.1456
Acta Physica Sinica
30
11
2005-07-29
//www.getgobooth.com/en/article/doi/10.7498/aps.30.1456
1456-1463
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//www.getgobooth.com/en/article/doi/10.7498/aps.30.1464
Author(s): JIANG YI-FENG, HUANG NAN-TANG, XU JI-REN, LIN GUANG-HAI <br/><p>The dependences of OAO fluorescence on space and time are investigated by using a time and space resolved method. The notable effect of the geometrical shape of the sample cell on OAO fluorescence is observed. A pulse acoustic wave and its relationship with OAO flurescence are recorded. It shows that the excited BC13 molecules are excited again becase of the action of the pulse acoustic wave By using of a simple model, the generation of OAO fluorescence and its axial shift are analysed. The calculated results are in agreement with the experimental data.</p> <br/>Acta Physica Sinica. 1981 30(11): 1464-1478. Published 2005-07-29
Author(s): JIANG YI-FENG, HUANG NAN-TANG, XU JI-REN, LIN GUANG-HAI <br/><p>The dependences of OAO fluorescence on space and time are investigated by using a time and space resolved method. The notable effect of the geometrical shape of the sample cell on OAO fluorescence is observed. A pulse acoustic wave and its relationship with OAO flurescence are recorded. It shows that the excited BC13 molecules are excited again becase of the action of the pulse acoustic wave By using of a simple model, the generation of OAO fluorescence and its axial shift are analysed. The calculated results are in agreement with the experimental data.</p> <br/>Acta Physica Sinica. 1981 30(11): 1464-1478. Published 2005-07-29
THE PULSE OPTICAL-ACOUSTIC-OPTICAL EFFECT OF VISIBLE FLUORESCENCE INDUCED BY INTENSE INFRARED LASER RADIATION IN BCl3 MOLECULES
JIANG YI-FENG, HUANG NAN-TANG, XU JI-REN, LIN GUANG-HAI
2005-07-29
Personal use only, all commercial or other reuse prohibited
Acta Physica Sinica. 1981 30(11): 1464-1478.
article
doi:10.7498/aps.30.1464
10.7498/aps.30.1464
Acta Physica Sinica
30
11
2005-07-29
//www.getgobooth.com/en/article/doi/10.7498/aps.30.1464
1464-1478
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//www.getgobooth.com/en/article/doi/10.7498/aps.30.1479
Author(s): QIAN ZU-WEN <br/><p>Atechnique for analytic evaluation of one-dimension Huygens' integral is proposed. The sound fields of the parametric line array can be analysed by it. Firstly, the point-source function is expanded into an operator on a plane wave function. Putting it into above mentioned integral and calculating it, it is shown that if we make an operation of this operator on the far-field solution, a general expression of radiation from parametric line array can be obtained. Secondly, both Fraunhofer's far-field approximation expression and Fresnel's, nearfield approximation expression are derived from it, but the latter approximation make a appreciable contribution on the radiation only outside the range of half-width angle.Furthermore; the radiation of a truncated parametric line array whose length is R1 is caleucated. We find that the beam pattern of this array becomes more narrow as decreasing the range. And a prediction can be made that the radiation field of a real parametric array will depend on following three parameters: kR sin2θ, βR, R1. Finally, basing on this theory, it appears to the author that the inconsistencies in ap-pearenee for some published experiments can be consistent with each other.</p> <br/>Acta Physica Sinica. 1981 30(11): 1479-1487. Published 2005-07-29
Author(s): QIAN ZU-WEN <br/><p>Atechnique for analytic evaluation of one-dimension Huygens' integral is proposed. The sound fields of the parametric line array can be analysed by it. Firstly, the point-source function is expanded into an operator on a plane wave function. Putting it into above mentioned integral and calculating it, it is shown that if we make an operation of this operator on the far-field solution, a general expression of radiation from parametric line array can be obtained. Secondly, both Fraunhofer's far-field approximation expression and Fresnel's, nearfield approximation expression are derived from it, but the latter approximation make a appreciable contribution on the radiation only outside the range of half-width angle.Furthermore; the radiation of a truncated parametric line array whose length is R1 is caleucated. We find that the beam pattern of this array becomes more narrow as decreasing the range. And a prediction can be made that the radiation field of a real parametric array will depend on following three parameters: kR sin2θ, βR, R1. Finally, basing on this theory, it appears to the author that the inconsistencies in ap-pearenee for some published experiments can be consistent with each other.</p> <br/>Acta Physica Sinica. 1981 30(11): 1479-1487. Published 2005-07-29
A NEW METHOD FOR CALCULATING RADIATION FROM PARAMETRIC LINE ARRAY
QIAN ZU-WEN
2005-07-29
Personal use only, all commercial or other reuse prohibited
Acta Physica Sinica. 1981 30(11): 1479-1487.
article
doi:10.7498/aps.30.1479
10.7498/aps.30.1479
Acta Physica Sinica
30
11
2005-07-29
//www.getgobooth.com/en/article/doi/10.7498/aps.30.1479
1479-1487
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//www.getgobooth.com/en/article/doi/10.7498/aps.30.1488
Author(s): LU XUE-SHAN, LUO SHOU-MIN <br/><p>The computer method of indexing Debye-Scherrer photographs has been extended to the case of orthorhombic crystals. Any observed diffraction line may be represented by an equation of a plane hi2A+ki2B+li2C=sin2θi in the A-B-C three dimensional space, where A, B, and C are related to the translational vectors a, b, and c by A = λ2/4a2. B = λ2/4b2, and C = λ2/4c2 respectively. Since the indices (hi, ki, li) are unknown at the outset, these planes are only conditional planes. It is seen that the intersection of three conditional planes, representing respectively three low angle lines with simple indices, will determine a point in the space which might indicate the dimensions of the unit cell. To guard against accidental coincidences, a series of equiatomic curved surfaces is introduced, representing in each case an integral number of configuration units contained in the unit cell. The equation of the equiatomic curved surface is ABC = (pλ3/8Mm0)2 (l/Z2), where p is the density of the crystal, M the formula weight of the configuration unit, m0 the mass of the atom of unit atomic weight, and Z the number of configuraunits contained therein, Z being a parameter. It is seen that if the point determined by the intersection of conditional planes is a physical point, this point must lie on one of the equiatomic surfaces.As a further discrimination, a fourth observed line may be used, to see whether a triplet (h, k, l) of the coefficients may be fitted into the conditional equation to form a plane that will pass through the proposed point.In fact, the whole geometrical problem is reduced to that all planes represented by their respective proper triplets will intersect at one point which passes through an equiatomic surface.The programme is written in Fortran and will be indicated by POWDBX-OR.</p> <br/>Acta Physica Sinica. 1981 30(11): 1488-1497. Published 2005-07-29
Author(s): LU XUE-SHAN, LUO SHOU-MIN <br/><p>The computer method of indexing Debye-Scherrer photographs has been extended to the case of orthorhombic crystals. Any observed diffraction line may be represented by an equation of a plane hi2A+ki2B+li2C=sin2θi in the A-B-C three dimensional space, where A, B, and C are related to the translational vectors a, b, and c by A = λ2/4a2. B = λ2/4b2, and C = λ2/4c2 respectively. Since the indices (hi, ki, li) are unknown at the outset, these planes are only conditional planes. It is seen that the intersection of three conditional planes, representing respectively three low angle lines with simple indices, will determine a point in the space which might indicate the dimensions of the unit cell. To guard against accidental coincidences, a series of equiatomic curved surfaces is introduced, representing in each case an integral number of configuration units contained in the unit cell. The equation of the equiatomic curved surface is ABC = (pλ3/8Mm0)2 (l/Z2), where p is the density of the crystal, M the formula weight of the configuration unit, m0 the mass of the atom of unit atomic weight, and Z the number of configuraunits contained therein, Z being a parameter. It is seen that if the point determined by the intersection of conditional planes is a physical point, this point must lie on one of the equiatomic surfaces.As a further discrimination, a fourth observed line may be used, to see whether a triplet (h, k, l) of the coefficients may be fitted into the conditional equation to form a plane that will pass through the proposed point.In fact, the whole geometrical problem is reduced to that all planes represented by their respective proper triplets will intersect at one point which passes through an equiatomic surface.The programme is written in Fortran and will be indicated by POWDBX-OR.</p> <br/>Acta Physica Sinica. 1981 30(11): 1488-1497. Published 2005-07-29
THE ALGORISM AND COMPUTER PROGRAMME FOR INDEXING ORTHORHOMBIC DEBYE-SCHERRER PHOTOGRAPHS
LU XUE-SHAN, LUO SHOU-MIN
2005-07-29
Personal use only, all commercial or other reuse prohibited
Acta Physica Sinica. 1981 30(11): 1488-1497.
article
doi:10.7498/aps.30.1488
10.7498/aps.30.1488
Acta Physica Sinica
30
11
2005-07-29
//www.getgobooth.com/en/article/doi/10.7498/aps.30.1488
1488-1497
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//www.getgobooth.com/en/article/doi/10.7498/aps.30.1498
Author(s): LU XUE-SHAN, LIANG JING-KUI <br/><p>As Debye chiracteristic temperature denotes the average vibration energy of atoms or ions in a costal, while different atoms in the crystal may have different vibration modes, or the same atom in a noncubie crystal may have different vibration modes along different directions, there arises the problem of inhomogeneity and anisotropy of characteristic temperatures.It is discussed in this paper the methods of investigating the inhomogeneity and anisotropy of characteristic temperatures in crystals.If there are two kinds of atoms (a) and (b) in a crystal, then the diffraction lines in the Debye-Scherrer photograph may be classified into two categories: in one of them the structure factor is the sum of the structure factors of respective atoms, F5= mFa + nFb, while in the other, the structure factor is the difference of the structure factors of respective atoms, F = gFa - qFd. Owing to the fact that both Fsobs and Fdobs are functions of sin θ/λ, so, if observed values of Fsobs and Fdobs are plotted against sin θ/λ, two smooth curves should be obtained, where Fobs= KFcalc. In the calculated structure factors, Fa= fa exp(-Ba sin2 θ/λ2) and Fb= fbexp(-Bb sin2θ/λ2), where fa and fb are the atomic scattering factors of the respective atoms, while Ba and Bb are Debye parameters of the respective atoms in the crystal. It is seen that from the two curves one can find the corresponding values of Fobsd or Fobss at the same abscissas as Fobss or Fobsd. If corresponding pairs of values are multiplied by proper coefficients and then be added or subtracted, a series of values of Fobs+ and obs- can be obtained which are now pure functions of Fa and Fb. Then if log (fa/Fobs+) and log (fb/Fobs-) are plotted agains sin2θ respectively, two straight lines can be obtained which should intercept at the same point on the ordinate axis, the slopes of which represent respectively Ba log e/λ2 and Bb log e/λ2, whence one can obtain Ba and Bb. For anisotropic crystals, a series of (h, k, 0) reflexions should be singled out. Just as in the case of isotropic crystals, one may plot log(Icalc/Iobs) against sin2θ, a straight line should be obtained, the slope of which gives 2B⊥ log e/λ2. Then single out another series of (0, 0, 1) reflexions. If one plots log (Icatc/Iobs) against sin2θ, then another straight line should be obtained, the slope of which gives 2B‖ log e/λ2. The two straight lines should intercept at the same point on the ordinate axis. Here B‖ and B⊥ represent the Debye parameters parallel and perpendicular to the principal axis respectively.Having datermined Debye parameters, characteristic temperatures can be obtained in the same way as we have described in our previous paper.The characteristic temperatures of CaF2 have been determined. It is shown that the characteristic temperature of Ca2+ ion in CaF2 crystals is 400K, while that of F-ion is 476K, the difference being 76K.</p> <br/>Acta Physica Sinica. 1981 30(11): 1498-1507. Published 2005-07-29
Author(s): LU XUE-SHAN, LIANG JING-KUI <br/><p>As Debye chiracteristic temperature denotes the average vibration energy of atoms or ions in a costal, while different atoms in the crystal may have different vibration modes, or the same atom in a noncubie crystal may have different vibration modes along different directions, there arises the problem of inhomogeneity and anisotropy of characteristic temperatures.It is discussed in this paper the methods of investigating the inhomogeneity and anisotropy of characteristic temperatures in crystals.If there are two kinds of atoms (a) and (b) in a crystal, then the diffraction lines in the Debye-Scherrer photograph may be classified into two categories: in one of them the structure factor is the sum of the structure factors of respective atoms, F5= mFa + nFb, while in the other, the structure factor is the difference of the structure factors of respective atoms, F = gFa - qFd. Owing to the fact that both Fsobs and Fdobs are functions of sin θ/λ, so, if observed values of Fsobs and Fdobs are plotted against sin θ/λ, two smooth curves should be obtained, where Fobs= KFcalc. In the calculated structure factors, Fa= fa exp(-Ba sin2 θ/λ2) and Fb= fbexp(-Bb sin2θ/λ2), where fa and fb are the atomic scattering factors of the respective atoms, while Ba and Bb are Debye parameters of the respective atoms in the crystal. It is seen that from the two curves one can find the corresponding values of Fobsd or Fobss at the same abscissas as Fobss or Fobsd. If corresponding pairs of values are multiplied by proper coefficients and then be added or subtracted, a series of values of Fobs+ and obs- can be obtained which are now pure functions of Fa and Fb. Then if log (fa/Fobs+) and log (fb/Fobs-) are plotted agains sin2θ respectively, two straight lines can be obtained which should intercept at the same point on the ordinate axis, the slopes of which represent respectively Ba log e/λ2 and Bb log e/λ2, whence one can obtain Ba and Bb. For anisotropic crystals, a series of (h, k, 0) reflexions should be singled out. Just as in the case of isotropic crystals, one may plot log(Icalc/Iobs) against sin2θ, a straight line should be obtained, the slope of which gives 2B⊥ log e/λ2. Then single out another series of (0, 0, 1) reflexions. If one plots log (Icatc/Iobs) against sin2θ, then another straight line should be obtained, the slope of which gives 2B‖ log e/λ2. The two straight lines should intercept at the same point on the ordinate axis. Here B‖ and B⊥ represent the Debye parameters parallel and perpendicular to the principal axis respectively.Having datermined Debye parameters, characteristic temperatures can be obtained in the same way as we have described in our previous paper.The characteristic temperatures of CaF2 have been determined. It is shown that the characteristic temperature of Ca2+ ion in CaF2 crystals is 400K, while that of F-ion is 476K, the difference being 76K.</p> <br/>Acta Physica Sinica. 1981 30(11): 1498-1507. Published 2005-07-29
THE INHOMOGENEITY AND ANISOTROPY OF DEBYE CHARACTERISTIC TEMPERATURES
LU XUE-SHAN, LIANG JING-KUI
2005-07-29
Personal use only, all commercial or other reuse prohibited
Acta Physica Sinica. 1981 30(11): 1498-1507.
article
doi:10.7498/aps.30.1498
10.7498/aps.30.1498
Acta Physica Sinica
30
11
2005-07-29
//www.getgobooth.com/en/article/doi/10.7498/aps.30.1498
1498-1507
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//www.getgobooth.com/en/article/doi/10.7498/aps.30.1508
Author(s): ZHAO ZHENG <br/><p>It has been proved in this paper that in general the horizons in 4-dimensional static Riemann spacetime will produce Hawking radiations and the radiative temperature is proportional to the surface gravity k of the horizon.This work is extended to the state that there exist electromagnetic fields. We point out that the static electric potential which effects Hawking radiative spectrum may originate from the electrie charge inside the hos,izoii as well as outside the hosizon.The Rindler radiations in uniform accelerated frames and the Hawking radiations from Schwarzsehild B. H., Keissner-Nordstrom B. H. as wall as Schwarzschild-de Sitter universe horizons are the special cases of our present general theory.It is pointed out that the equivalence principle Is still effective and Rindlerradiations do originate from the horizons of the Rindler frames of reference. Hawkingradiation only has relation with dynamic effect K near the horizon, but has no relation with curvature of the spaeetime.</p> <br/>Acta Physica Sinica. 1981 30(11): 1508-1519. Published 2005-07-29
Author(s): ZHAO ZHENG <br/><p>It has been proved in this paper that in general the horizons in 4-dimensional static Riemann spacetime will produce Hawking radiations and the radiative temperature is proportional to the surface gravity k of the horizon.This work is extended to the state that there exist electromagnetic fields. We point out that the static electric potential which effects Hawking radiative spectrum may originate from the electrie charge inside the hos,izoii as well as outside the hosizon.The Rindler radiations in uniform accelerated frames and the Hawking radiations from Schwarzsehild B. H., Keissner-Nordstrom B. H. as wall as Schwarzschild-de Sitter universe horizons are the special cases of our present general theory.It is pointed out that the equivalence principle Is still effective and Rindlerradiations do originate from the horizons of the Rindler frames of reference. Hawkingradiation only has relation with dynamic effect K near the horizon, but has no relation with curvature of the spaeetime.</p> <br/>Acta Physica Sinica. 1981 30(11): 1508-1519. Published 2005-07-29
HAWKING RADIATION IN FOUR DIMENSIONAL STATIC RIEMANN SPACETIME
ZHAO ZHENG
2005-07-29
Personal use only, all commercial or other reuse prohibited
Acta Physica Sinica. 1981 30(11): 1508-1519.
article
doi:10.7498/aps.30.1508
10.7498/aps.30.1508
Acta Physica Sinica
30
11
2005-07-29
//www.getgobooth.com/en/article/doi/10.7498/aps.30.1508
1508-1519
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//www.getgobooth.com/en/article/doi/10.7498/aps.30.1520
Author(s): WANG YONG-ZHONG <br/><p>Some formulae of the empirical coefficient method in fluorescent X-ray spectrometric analysis are discussed theoretically and a general formula is obtained thereupon. The physical significance of the coefficients used is explained. A formula based upon the calculation of relative intensity of fluorescent X-ray is derived and it is relatively simple in application.</p> <br/>Acta Physica Sinica. 1981 30(11): 1520-1527. Published 2005-07-29
Author(s): WANG YONG-ZHONG <br/><p>Some formulae of the empirical coefficient method in fluorescent X-ray spectrometric analysis are discussed theoretically and a general formula is obtained thereupon. The physical significance of the coefficients used is explained. A formula based upon the calculation of relative intensity of fluorescent X-ray is derived and it is relatively simple in application.</p> <br/>Acta Physica Sinica. 1981 30(11): 1520-1527. Published 2005-07-29
THEORETICAL ANALYSIS OF THE EMPIRICAL COEFFICIENT METHODS FOR FLUORESCENT X-RAY SPECTROMETRY
WANG YONG-ZHONG
2005-07-29
Personal use only, all commercial or other reuse prohibited
Acta Physica Sinica. 1981 30(11): 1520-1527.
article
doi:10.7498/aps.30.1520
10.7498/aps.30.1520
Acta Physica Sinica
30
11
2005-07-29
//www.getgobooth.com/en/article/doi/10.7498/aps.30.1520
1520-1527
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//www.getgobooth.com/en/article/doi/10.7498/aps.30.1528
Author(s): LING BING-CHANG <br/><p>This paper discusses Takagi equation by means of perturbation methods. A perturbative solution of diffraction amplitude in slightly deformation crystal is obtained for the spherical incident wave.</p> <br/>Acta Physica Sinica. 1981 30(11): 1528-1532. Published 2005-07-29
Author(s): LING BING-CHANG <br/><p>This paper discusses Takagi equation by means of perturbation methods. A perturbative solution of diffraction amplitude in slightly deformation crystal is obtained for the spherical incident wave.</p> <br/>Acta Physica Sinica. 1981 30(11): 1528-1532. Published 2005-07-29
PERTURBATIVE SOLUTION OF TAKAGI EQUATION IN X-RAY DIFFRACTION DYNAMIC IN SLIGHTLY DEFORMATION CRYSTAL
LING BING-CHANG
2005-07-29
Personal use only, all commercial or other reuse prohibited
Acta Physica Sinica. 1981 30(11): 1528-1532.
article
doi:10.7498/aps.30.1528
10.7498/aps.30.1528
Acta Physica Sinica
30
11
2005-07-29
//www.getgobooth.com/en/article/doi/10.7498/aps.30.1528
1528-1532
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//www.getgobooth.com/en/article/doi/10.7498/aps.30.1533
Author(s): LIU WEN-XI, ZHAO CHANG-AN <br/><p>A new indexing method on the spots of high order Lane zone in electron diffraction pattern has been developed. The first spot indices of high order Laue zone are determined immediately by means of measuring the distances between the bright dif-feraction spots and a vector composition procedure the indices of the spot closest to the centre and other spots are then derived.</p> <br/>Acta Physica Sinica. 1981 30(11): 1533-1538. Published 2005-07-29
Author(s): LIU WEN-XI, ZHAO CHANG-AN <br/><p>A new indexing method on the spots of high order Lane zone in electron diffraction pattern has been developed. The first spot indices of high order Laue zone are determined immediately by means of measuring the distances between the bright dif-feraction spots and a vector composition procedure the indices of the spot closest to the centre and other spots are then derived.</p> <br/>Acta Physica Sinica. 1981 30(11): 1533-1538. Published 2005-07-29
INDEXING OF HIGH ORDER LAUE SPOTS BY A DIFFERENCE VECTOR METHOD
LIU WEN-XI, ZHAO CHANG-AN
2005-07-29
Personal use only, all commercial or other reuse prohibited
Acta Physica Sinica. 1981 30(11): 1533-1538.
article
doi:10.7498/aps.30.1533
10.7498/aps.30.1533
Acta Physica Sinica
30
11
2005-07-29
//www.getgobooth.com/en/article/doi/10.7498/aps.30.1533
1533-1538
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//www.getgobooth.com/en/article/doi/10.7498/aps.30.1539
Author(s): FAN HAI-FU <br/><p>Difference structures are structures subjected to certain mathematical processing, they are introduced for the convenience of solving heavy-atom-containing structures by direct methods. Information about the arrangement of light atoms can be obtained by solving the corresponding difference structure. However the existing methods of solving difference structures have not yet made full use of the angular parts of the heavy-atom contribution. In this paper an improved method is given in this respect.</p> <br/>Acta Physica Sinica. 1981 30(11): 1539-1542. Published 2005-07-29
Author(s): FAN HAI-FU <br/><p>Difference structures are structures subjected to certain mathematical processing, they are introduced for the convenience of solving heavy-atom-containing structures by direct methods. Information about the arrangement of light atoms can be obtained by solving the corresponding difference structure. However the existing methods of solving difference structures have not yet made full use of the angular parts of the heavy-atom contribution. In this paper an improved method is given in this respect.</p> <br/>Acta Physica Sinica. 1981 30(11): 1539-1542. Published 2005-07-29
AN IMPROVED PROCEDURE OF SOLVING DIFFERENCE STRUCTURES
FAN HAI-FU
2005-07-29
Personal use only, all commercial or other reuse prohibited
Acta Physica Sinica. 1981 30(11): 1539-1542.
article
doi:10.7498/aps.30.1539
10.7498/aps.30.1539
Acta Physica Sinica
30
11
2005-07-29
//www.getgobooth.com/en/article/doi/10.7498/aps.30.1539
1539-1542
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//www.getgobooth.com/en/article/doi/10.7498/aps.30.1543
Author(s): TU JIN-LIANG, WU YAO-AN, TANG YUAN-FENG, SUN JIN-MEI, FENG LIN-TING, LI JING-LONG, LIAO JING-YING, WU HUI-FA, XU HUI-DE <br/><p>The growth and characterization of BNN crystals had been investigated and the large BNN crystals with SH output power level greater than 1 watt (the highest output being 2.5 watt) had been grown successfully.</p> <br/>Acta Physica Sinica. 1981 30(11): 1543-1547. Published 2005-07-29
Author(s): TU JIN-LIANG, WU YAO-AN, TANG YUAN-FENG, SUN JIN-MEI, FENG LIN-TING, LI JING-LONG, LIAO JING-YING, WU HUI-FA, XU HUI-DE <br/><p>The growth and characterization of BNN crystals had been investigated and the large BNN crystals with SH output power level greater than 1 watt (the highest output being 2.5 watt) had been grown successfully.</p> <br/>Acta Physica Sinica. 1981 30(11): 1543-1547. Published 2005-07-29
CRYSTAL GROWTH AND CHARACTERIZATION OF BARIUM SODIUM NIOBATE WITH HIGH SH OUTPUT
TU JIN-LIANG, WU YAO-AN, TANG YUAN-FENG, SUN JIN-MEI, FENG LIN-TING, LI JING-LONG, LIAO JING-YING, WU HUI-FA, XU HUI-DE
2005-07-29
Personal use only, all commercial or other reuse prohibited
Acta Physica Sinica. 1981 30(11): 1543-1547.
article
doi:10.7498/aps.30.1543
10.7498/aps.30.1543
Acta Physica Sinica
30
11
2005-07-29
//www.getgobooth.com/en/article/doi/10.7498/aps.30.1543
1543-1547
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//www.getgobooth.com/en/article/doi/10.7498/aps.30.1548
Author(s): LAN GUO-XIANG, LI GUAN-GAO, LI BING, WANG HUA-FU <br/><p>The Raman spectra of LiTaO3 have been studied from 20℃ to 800℃. No softening of ferroelectric mode has been detected. The striking feature of our results is that the Raman spectra of the ferroelectric phase merge into the paraelectric phase without any appreciable discontinuity at the phase transition. On the basis of these new experimental results and the crystal structure data in literature, we suggest that the ferroelectric phase transition in LiTaO3 may have an order-disorder character.</p> <br/>Acta Physica Sinica. 1981 30(11): 1548-1553. Published 2005-07-29
Author(s): LAN GUO-XIANG, LI GUAN-GAO, LI BING, WANG HUA-FU <br/><p>The Raman spectra of LiTaO3 have been studied from 20℃ to 800℃. No softening of ferroelectric mode has been detected. The striking feature of our results is that the Raman spectra of the ferroelectric phase merge into the paraelectric phase without any appreciable discontinuity at the phase transition. On the basis of these new experimental results and the crystal structure data in literature, we suggest that the ferroelectric phase transition in LiTaO3 may have an order-disorder character.</p> <br/>Acta Physica Sinica. 1981 30(11): 1548-1553. Published 2005-07-29
RAMAN SPECTRA STUDY OF FERROELECTRIC PHASE TRANSITION IN LiTaO3
LAN GUO-XIANG, LI GUAN-GAO, LI BING, WANG HUA-FU
2005-07-29
Personal use only, all commercial or other reuse prohibited
Acta Physica Sinica. 1981 30(11): 1548-1553.
article
doi:10.7498/aps.30.1548
10.7498/aps.30.1548
Acta Physica Sinica
30
11
2005-07-29
//www.getgobooth.com/en/article/doi/10.7498/aps.30.1548
1548-1553
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//www.getgobooth.com/en/article/doi/10.7498/aps.30.1554
Author(s): WANG HUAN-YUAN, ZHANG PENG-XIANG, ZHANG XU-XIN, XU XIAO-ZHEN <br/><p>Polar Kerr rotation (PKR) spectra of Bi-substituted YIG monocrystals, grown by flux method, were measured in the wave length region of 0.4 to 0.8 μm at room temperature. The natural grown surfaces, as well as surfaces newly cut across different parts of the crystals were all taken under examination. The variations in the height of the same characterizing peak near 2.7 eV reveal the imhomogeneity of the content of Bi ions, entering the dodecahedral site of the lattice. Our work demonstrates the possibility of PKR spectra as a tool of surface layer analysis, applicable in the investigation of such processes as ionic distribution, diffusion or surface segregation.</p> <br/>Acta Physica Sinica. 1981 30(11): 1554-1558. Published 2005-07-29
Author(s): WANG HUAN-YUAN, ZHANG PENG-XIANG, ZHANG XU-XIN, XU XIAO-ZHEN <br/><p>Polar Kerr rotation (PKR) spectra of Bi-substituted YIG monocrystals, grown by flux method, were measured in the wave length region of 0.4 to 0.8 μm at room temperature. The natural grown surfaces, as well as surfaces newly cut across different parts of the crystals were all taken under examination. The variations in the height of the same characterizing peak near 2.7 eV reveal the imhomogeneity of the content of Bi ions, entering the dodecahedral site of the lattice. Our work demonstrates the possibility of PKR spectra as a tool of surface layer analysis, applicable in the investigation of such processes as ionic distribution, diffusion or surface segregation.</p> <br/>Acta Physica Sinica. 1981 30(11): 1554-1558. Published 2005-07-29
KERR ROTATION IN THE BI-YIG MONOCRYSTALS
WANG HUAN-YUAN, ZHANG PENG-XIANG, ZHANG XU-XIN, XU XIAO-ZHEN
2005-07-29
Personal use only, all commercial or other reuse prohibited
Acta Physica Sinica. 1981 30(11): 1554-1558.
article
doi:10.7498/aps.30.1554
10.7498/aps.30.1554
Acta Physica Sinica
30
11
2005-07-29
//www.getgobooth.com/en/article/doi/10.7498/aps.30.1554
1554-1558
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//www.getgobooth.com/en/article/doi/10.7498/aps.30.1559
Author(s): QIAN ZU-WEN <br/><p>In this paper, it has been shown that in the near field of parametric sound array, the Fresnel's approximation proposed by Berktay is inappropriate.</p> <br/>Acta Physica Sinica. 1981 30(11): 1559-1561. Published 2005-07-29
Author(s): QIAN ZU-WEN <br/><p>In this paper, it has been shown that in the near field of parametric sound array, the Fresnel's approximation proposed by Berktay is inappropriate.</p> <br/>Acta Physica Sinica. 1981 30(11): 1559-1561. Published 2005-07-29
ON THE NEAR FIELD OF PARAMETRIC SOUND ARRAY
QIAN ZU-WEN
2005-07-29
Personal use only, all commercial or other reuse prohibited
Acta Physica Sinica. 1981 30(11): 1559-1561.
article
doi:10.7498/aps.30.1559
10.7498/aps.30.1559
Acta Physica Sinica
30
11
2005-07-29
//www.getgobooth.com/en/article/doi/10.7498/aps.30.1559
1559-1561
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//www.getgobooth.com/en/article/doi/10.7498/aps.30.1562
Author(s): AN YING, CHEN SHI, GUO HAN-YING <br/><p>A U1-bundle formalism for the Born-Infeld electrodynamics is proposed and the equation of motion for a test particle in the Born-Infeld electromagnetic field is given. There are two forces acting on the test particle, one corresponds to the Lorentz force and the other the Poincaré stress.</p> <br/>Acta Physica Sinica. 1981 30(11): 1562-1564. Published 2005-07-29
Author(s): AN YING, CHEN SHI, GUO HAN-YING <br/><p>A U1-bundle formalism for the Born-Infeld electrodynamics is proposed and the equation of motion for a test particle in the Born-Infeld electromagnetic field is given. There are two forces acting on the test particle, one corresponds to the Lorentz force and the other the Poincaré stress.</p> <br/>Acta Physica Sinica. 1981 30(11): 1562-1564. Published 2005-07-29
A U1 PRINCIPAL BUNDLE THEORY FOR THE BORN-INFELD ELECTRODYNAMICS
AN YING, CHEN SHI, GUO HAN-YING
2005-07-29
Personal use only, all commercial or other reuse prohibited
Acta Physica Sinica. 1981 30(11): 1562-1564.
article
doi:10.7498/aps.30.1562
10.7498/aps.30.1562
Acta Physica Sinica
30
11
2005-07-29
//www.getgobooth.com/en/article/doi/10.7498/aps.30.1562
1562-1564
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//www.getgobooth.com/en/article/doi/10.7498/aps.30.1565
Author(s): ZHANG YANG-ZHONG <br/><p>By using the perturbative expansions of 〈j⊥· E⊥〉 it was proved that the coherent renormalization theory acquired the energy conservation of non-linear drift waves within the sixth order.</p> <br/>Acta Physica Sinica. 1981 30(11): 1565-1568. Published 2005-07-29
Author(s): ZHANG YANG-ZHONG <br/><p>By using the perturbative expansions of 〈j⊥· E⊥〉 it was proved that the coherent renormalization theory acquired the energy conservation of non-linear drift waves within the sixth order.</p> <br/>Acta Physica Sinica. 1981 30(11): 1565-1568. Published 2005-07-29
ENERGY CONSERVATION OF NON-LINEAR DRIFT WAVES IN THE COHERENT RENORMALIZATION
ZHANG YANG-ZHONG
2005-07-29
Personal use only, all commercial or other reuse prohibited
Acta Physica Sinica. 1981 30(11): 1565-1568.
article
doi:10.7498/aps.30.1565
10.7498/aps.30.1565
Acta Physica Sinica
30
11
2005-07-29
//www.getgobooth.com/en/article/doi/10.7498/aps.30.1565
1565-1568