-
Yoko Miyatake
1980 Volume 48 Issue 3 Pages
711-719
Published: March 15, 1980
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The results of the β-γ directional correlation measurement of the first-forbidden β-transition of
149Pm showed a slight energy dependence in the reduced β-coefficient ratio,
R(
Ei)⁄
R(
Ek), impling a deviation from the ξ-approximation. The analysis is based on the theoretical expressions given by Morita and Morita and performed by the minimization of χ
2 for the directional correlation coefficient ratio,
A2(
Ei)⁄
A2(
Ek). Two sets of the nuclear matrix parameters and corresponding values of the γ-coefficient,
A2γ, and E2 mixing of the 286 keV transition were found: set I,
x=−0.119±0.140,
u=−1.545±0.160,
y′=−15.46±1.57,
A2γ=0.09±0.12, 0.2%<E2<3.1%; set II,
x=0.795±0.136,
u=−1.363±0.126,
y′=23.41±1.42,
A2γ=−0.61±0.11, 19.4%<E2<37.8%. Set I is tentatively preferred. The deviation from the ξ-approximation is interpreted in terms of the effect of cancellation among the parameters.
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Seigo Koh, Koichi Nakayama, Minoru Tsuda, Toshifumi Hayashi, Yasutoshi ...
1980 Volume 48 Issue 3 Pages
720-727
Published: March 15, 1980
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The
26Mg(d, p)
27Mg neutron stripping reaction has been studied at 3.1 and 3.5 MeV. Product protons corresponding to levels up to 4.8 MeV in
27Mg were analysed with the broad range magnetic spectrograph with peak widths of ∼7 keV (FWHM) at eight angles from θ=15° to θ=120°. Cross sections are analysed using the DWBA theory and the statistical theory of Hauser and Feshbach. The angular momentum transfers
ln are determined undoubtfully. The spectroscopic factors for respective states are then compared with the shell model calculations of Wildenthal
et al. and the predictions of the collective model.
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Osamu Sakai
1980 Volume 48 Issue 3 Pages
728-737
Published: March 15, 1980
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The electronic structure in the mixed valence state in the case that one of two different valence states has a singlet
LSJ level is studied here. This study is based on the multisite Friedel-Anderson model with the spin-orbit interaction. The alloy analogy of Hubbard is used to treat the effects of strong correlations. The susceptibility is calculated as a function of temperature. It has a maximum at a low temperature and is finite as
T→0 K. A gap or a dip appears around the
f level in the density of states of the conduction electrons.
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Yoshitsugu Oono, Tohru Kohda, Hideki Yamazaki
1980 Volume 48 Issue 3 Pages
738-745
Published: March 15, 1980
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As a possible dual concept of the order parameter in the theory of phase transition, it is desirable to introduce the disorder parameter for chaos. A mathematically well-defined disorder parameter is proposed, which is presumably identical with the Kolumogorov entropy, though rigorous proof is not yet obtained. Possible potential applications of the disorder parameter to the analyses of time-series are given.
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Minoru Takahashi
1980 Volume 48 Issue 3 Pages
746-750
Published: March 15, 1980
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It is shown that the motion of the plane rotator model should be described by a set of equations
(
Remark: Graphics omitted.),
i=1, 2, ···,
N,
and that the Hamiltonian should be
(
Remark: Graphics omitted.).
To this Hamiltonian one can apply the method of molecular dynamics. For the case of the nearest neighbor interaction, energy-temperature curve is calculated for one, two and three dimensions. In one dimension our result agrees well with the exact solution. In two dimension a sharp peak of specific heat is found at
T∼1.1
J⁄
k. In three dimension a singularity is observed at
T∼2.2
J⁄
k.
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Koji Muramatsu, Takehiko Oguchi
1980 Volume 48 Issue 3 Pages
751-756
Published: March 15, 1980
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Cluster approximation for the antiferromagnets is improved by extending the effective Hamiltonian method so that there appears no anti-Néel point. It is applied to the
S=1⁄2 antiferromagnet on a square lattice with anisotropic exchange interaction which includes the anisotropy parameter η. This system is reduced to the Heisenberg model or to the Ising model according as η goes to 1 or 0. The variations of the Néel point
TN and the specific heat with η are calculated. The results of the specific heat curves for η\gtrsim0.9 exhibit a broad maximum above
TN where a small spike appears.
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Katsuyuki Awa, Takashi Asahi
1980 Volume 48 Issue 3 Pages
757-761
Published: March 15, 1980
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The effect of correlations on polarizations in an electron gas is studied. The proper polarization is constructed from direct- and exchange-processes consisting of particle-particle ladder-vertices with a screened interaction. The short-wavelength behavior of the so-called local field correction
G(
p) is discussed.
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Kêitsiro Aizu
1980 Volume 48 Issue 3 Pages
762-765
Published: March 15, 1980
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Firstly the meaning of catastrophe indices and of the “fourth” checkpoint for second-order transitions are explained over again. And then three new theorems are presented. The first of them is most fundamental from which the two others follow. The second theorem is: The catastrophe indices of a transition parameter system always include a unity. The third theorem is: If the dimensionality of the irreducible representation for the transition parameters is lower than 3, the transition from the prototypic to a ferroic phase always passes the “fourth” checkpoint.
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Yasuaki Hiwatari, Akira Ueda
1980 Volume 48 Issue 3 Pages
766-772
Published: March 15, 1980
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A simple version for superionic conductors, of the soft-core model for simple liquids is proposed. That is, the model potential is composed of only the soft-core and the Coulomb potentials. Monte Carlo simulations for α-AgI are made with a fine-grained lattice for a 108-ion system at several temperatures. Sublattice disordering of cations is observed for an appropriate temperature range. At lower temperature the bcc lattice of anions becomes unstable and changes to an fcc-like structure, and at the same time cations show almost localized motions. These results are consistent with the experiments for AgI. The characteristics of the resulting structural properties for cations are also found to be consistent with the recent experimental results.
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Masaki Aihara
1980 Volume 48 Issue 3 Pages
773-779
Published: March 15, 1980
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We investigate the time-dependent polarization characteristics associated with resonance Raman scattering in a linearly-coupled localized-electron phonon system with a doubly-degenerate excited electronic level. It is found that the temporal polarization behavior for the pulse excitation strongly reflects the dynamics of the electron-phonon interaction in the intermediate state. In the case of a short pulse limit, the time-dependent degree of polarization (DP) exhibits the damped oscillation which is directly related to the dynamical motion of the interaction mode. For a square pulse with a finite pulse width, the interference effect between the scattering and the luminescence appears in the oscillatory behavior of DP during the excitation, and strongly depends on the incident photon energy.
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Kenji Takanaka, Tomitaro Nagashima
1980 Volume 48 Issue 3 Pages
780-785
Published: March 15, 1980
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A theoretical investigation has been carried out of the magnetization
M of type-II superconductors with cubic crystal symmetry. An explicit expression for
M is obtained near the transition temperature
Tc in the case where the applied field is slightly smaller than the upper critical field
Hc2. The obtained expression for
M consists of two cubic harmonics.
From consideration of the free energy, it is shown in a unified manner that the components of the magnetization parallel and perpendicular to the applied field
H0 are related to the anisotropy of the upper critical field
Hc2 or the lower critical field
Hc1 when
H0∼
Hc2 or
H0∼
Hc1 irrespective of the temperature.
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Shinji Wada, Syunzaburou Nakamura, Ryozo Aoki, Philippe Molinie
1980 Volume 48 Issue 3 Pages
786-792
Published: March 15, 1980
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Measurements of the
181Ta and
93Nb spin-lattice relaxation time
T1 at low temperatures are reported for the 2H polytypes of TaS
2 and NbS
2 and their pyridine intercalation compounds. An analysis of
T1T shows that, on the intercalation of pyridine molecules, the density of states at Fermi level
N(
EF) increases about 30% for 2H-TaS
2, while decreases about 30% for 2H-NbS
2. This is suggestive of charge transfer from pyridine molecules to
dz2 conduction band of the disulfides.
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Masakazu Ichiyanagi
1980 Volume 48 Issue 3 Pages
793-798
Published: March 15, 1980
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A Boss system has two broken symmetries, namely the gauge symmetry and the Galilei translation symmetry. We discuss the microscopic background of the ansatz that the superfluid flow is the manifestation of the local gauge invariance. To do this we show that the depletion velocity fields are the Goldstone fields due to the breakdown of the Galilei translation symmetry. A connection between a Bose-Einstein condensation and superfluid flow is also discussed.
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Kazushige Machida, Takeo Matsubara
1980 Volume 48 Issue 3 Pages
799-804
Published: March 15, 1980
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Possible magnetic instability in magnetic superconductors is studied by calculating the wave number dependent susceptibility χ(
q) in the presence of superconductivity. Effects of Fermi surface nesting on χ(
q) are examined for three models: Free electron gas model and tightly binding cosine band model of one-dimension, and Liu’s model for imperfect nesting. All model calculations reveal that stable magnetic ordering which coexists with superconductivity is antiferromagnetic one. Possibility of an incommensurate spin density wave state is discussed.
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Masao Shimizu
1980 Volume 48 Issue 3 Pages
805-813
Published: March 15, 1980
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The origin of the magnetic inhomogeneity in Fe–Ni Invar alloys is attributed to the first-order magnetic transition, which was predicted before in the itinerant electron model. The large effect of the magnetovolume coupling on various thermodynamic properties is examined in the model of magnetic mixing of the ferromagnetic phase with larger atomic volume and the paramagnetic phase with smaller atomic volume. At low temperatures the mixing is assumed to be frozen in. The mutual transformation between the ferromagnetic and paramagnetic phases due to the changes of temperature, magnetic field and pressure give additional contributions to the respective thermodynamic properties. The difference between the observed values of the field derivative of the volume and the pressure derivative of the magnetization is discussed. The experimental results of various thermodynamic properties in Fe–Ni Invar alloys are analyzed in connection with the present theoretical results and are satisfactorily explained.
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Shoji Ishida, Yasunori Kubo, Junji Ishida, Setsuro Asano
1980 Volume 48 Issue 3 Pages
814-821
Published: March 15, 1980
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In order to see the characteristic properties of the ferromagnetic Heusler alloys,the electronic structures of Ni
2MnSn and Pd
2MnSn have been calculated. The common properties of these alloys have been discussed by the present results and those obtained for Cu
2MnAl. The spin polarizations of the constituent atoms are in good are in good agreement with experimental ones. The signs of the spin polarizations of the
s-type conduction electrons in the inscribed spheres are consistent with the signs of the measured internal magnetic fields due to the conduction electrons.
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When Shan Chan, Katsuya Mitsuoka, Hideki Miyajima, Soshin Chikazumi
1980 Volume 48 Issue 3 Pages
822-829
Published: March 15, 1980
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Saturation magnetization, Curie temperature, magnetocrystalline anisotropy and magnetostriction were measured for M
1−cTi
c (M=Fe, Co, Ni) systems. The rate of change in saturation magnetic moment dμ⁄d
c at 0 K was found to be −6.2 μ
B and −4.3 μ
B per atom in Co–Ti and Ni–Ti systems, respectively. For Fe–Ti system the decrease in magnetic moment was non-linear. Curie temperatures of Ni–Ti system decrease monotonically at the rate of −42 K per atomic percent Ti and those of Fe–Ti system increase linearly at the rate of +3.7 K per atomic percent Ti. Magnetostriction and magnetocrystalline anisotropy of Fe–Ti system also increase with increasing Ti concentration.
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Hidetoshi Hiroyoshi, Akira Hoshi, Hiroyasu Fujimori, Yasuaki Nakagawa
1980 Volume 48 Issue 3 Pages
830-835
Published: March 15, 1980
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Magnetizations of pure Ni, 10 at% Cu–Ni, 10 at% Co–Ni, 46 at% Fe–Ni and amorphous 16 at% B–Fe alloys have been measured in static magnetic fields up to 100 kOe in the temperature range around the Curie points. The relation between magnetization
M, field
H and temperature
T is satisfactorily fitted to an equation (
H⁄
M)
0.75=
a(
T−
Tc)+
bM2.5 for all the alloys investigated, where
a and
b are constant parameters and
Tc is the Curie temperature. Accordingly, isotherms of the Arrott-Noakes plots,
M2.5 vs (
H⁄
M)
0.75, are parallel straight lines.
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Kohji Eguchi, Hironobu Fujii, Akio Mishima, Hiroshi Fujiwara, Tetsuhik ...
1980 Volume 48 Issue 3 Pages
836-842
Published: March 15, 1980
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Measurements of the magnetization and the magnetic susceptibility have been made along the principal axes of Dy–Th single crystal alloys with the hexagonal close-packed structure. The alloys exhibit a ferromagnetic structure at low temperatures in all composition region and screw antiferromagnetism appears in the sequence of the increase of the temperature in the composition less than about 12 at% Th. Magnetic transition temperatures
Tc and
TN increase and decrease with increasing Th concentration, respectively. The magnetocrystalline anisotropy constant
K20 was determined from the analysis of the hard magnetization curve. And the exchange interaction constant
j(
Q) was determined from the magnetic transition temperatures, and
j(0) and the magnetocrystalline anisotropy constant
K20 para in the paramagnetic state were also determined from the analysis of the paramagnetic susceptibility, respectively, on the basis of the molecular field theory.
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Fumihisa Ono
1980 Volume 48 Issue 3 Pages
843-849
Published: March 15, 1980
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Disordered Fe–Pt Invar alloys (around 30 at% Pt) show anomalous properties in both temperature and magnetic field dependences of the magneto-crystalline anisotropy constant
K1. A theory has been proposed based on the itinerant electron model by assuming a strong relationship between
K1 and the Fermi level of the minority spin band. The temperature dependence of
K1 can be explained by using the present theory. The decrease of the absolute value of
K1 with increasing the external field can also be explained by the present theory.
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Nozomu Inoue, Hiroshi Yasuoka, Shinji Ogawa
1980 Volume 48 Issue 3 Pages
850-856
Published: March 15, 1980
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The magnetic properties of a pyrite compound NiSe
2 have been investigated by the
77Se NMR, the magnetic susceptibility and the specific heat measurements in the temperature range between 1.6 and 300 K. The electronic specific heat coefficient, γ, is obtained to be (8.5±1.0) mJ/K
2mol. The values of the magnetic susceptibility and the Knight shift are estimated to be 2.17×10
−4 emu/mol and +(1.0±0.1)%, respectively, both being independent of temperature. The product of the nuclear spin-lattice relaxation time and temperature,
T1T, is found to be constant with a value or 240 msec K. From these results, it is concluded that NiSe
2 is one of the typical Pauli paramagnets and the usual Korringa relation holds with a relatively small exchange enhancement effect. Discussions of the origin of the hyperfine coupling constant of
77Se are also given in conjunction with the reported result of CoSe
2.
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Gendo Oomi
1980 Volume 48 Issue 3 Pages
857-864
Published: March 15, 1980
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The γ–α transition pressure (
Pγ–α), temperature (
Tγ–α), and critical point (
Pc,
Tc) of Ce
1−xLa
x alloys (
x=0.0∼0.03) were determined by electrical resistivity measurements under pressure up to 10 kbar at temperatures between 50 K and 300 K. A nonlinear dependence of
Tγ–α on pressure was confirmed for
x=0.0 and 0.02 in agreement with the theory for
x=0.0 by Miyamoto and Nagamiya (MN) rather than that by Ramirez and Falicov (RF). The impurity effects of lanthanum on
Pγ→α,
Tγ→α, and
Tα→γ were determined experimentally: ∂
Pγ→α⁄∂
x=(0.37±0.06)kbar/(at.%La), ∂
Tγ→α⁄∂
x=−(12.5±1)K/(at.%La) and ∂
Tα→γ⁄∂
x=−(12±1)K/(at.%La) respectively. These experimental results were found to be in qualitative agreement with the calculated results by an extension of the MN theory.
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Shojiro Mori, Tsuneya Ando
1980 Volume 48 Issue 3 Pages
865-873
Published: March 15, 1980
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Low temperature mobilities parallel to the layers of a heavily doped n-type GaAs-Ga
1−xAl
xAs superlattice are calculated as a function of carrier concentrations. Assumed scattering mechanisms are Coulomb scattering from donor ions and surface roughness scattering at the interface. The subband structure in the presence of the band bending is calculated by the variational method. The surface roughness scattering is shown to be relatively unimportant and the Coulomb scattering is dominant. The mobility in the modulation doping case becomes nearly one order of magnitude larger than that in the uniform doping case in agreement with recent experiments. The band bending effect is important in the modulation doping case and reduce the mobility at large carrier concentrations. The intersubband scattering greatly reduces the mobility when electrons occupy higher subbands.
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Masayoshi Yamada, Tatsutetsu Shirai, Keiichi Yamamoto, Kenji Abe
1980 Volume 48 Issue 3 Pages
874-881
Published: March 15, 1980
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The first observation of thermal Brillouin spectra in CdIn
2S
4 single crystals has been made at room temperature by using a sensitive photon-counting system, a piezoelectrically scanned Fabry-Perot interferometer and a He–Ne laser with the radiation wavelength of 632.8 nm. Brillouin doublets by acoustic phonons propagating along the [1, 0, 0], [1, 1, \sqrt2] and [\sqrt2+1, 1, 0] directions are observed at the 90°-scattering configuration and assigned to specific modes of vibration according to the polarization selection rule in Brillouin scattering. The elastic constants are determined from Brillouin shifts. The absolute photoelastic constants are obtained by the comparison of Brillouin intensities measured in CdIn
2S
4 with those in fused quartz under the same experimental conditions. The results are:
C11=12.15±0.10,
C12=2.46±0.46, and
C44=2.57±0.05 in unit of 10
10 N/m
2, and
P11=0.027±0.006,
P12=0.093±0.005, and
P44=−0.033±0.002.
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Tsutomu Nakamura, Masaru Kasahara, Itaru Tatsuzaki
1980 Volume 48 Issue 3 Pages
882-885
Published: March 15, 1980
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Proton spin-lattice relaxation time
T1 was measured in the temperature range from 10 to −170°C. Results obtained in the paraelectric phase were analyzed by assuming that the relaxation is caused by three mechanisms: diffusion motion of H
2O molecules, the hindered rotation of CH
3 and NH
3 radicals and the fluctuation of the local magnetic field which increases near the phase transition temperature owing to the critical slowing down of the order parameter. The relaxation rate caused by the third mechanism was found to depend on temperature as ln (
T−
T0), where
T0 is the paraelectric Curie temperature.
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Kazuo Gesi
1980 Volume 48 Issue 3 Pages
886-889
Published: March 15, 1980
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Dielectric constants were measured for the pseudo-hexagonal
c-plates of K
3H(SO
4)
2, Rb
3H(SO
4)
2, and their deuterated analogues below room temperature. The dielectric constants of K
3H(SO
4)
2 and Rb
3H(SO
4)
2 monotonically increase with decreasing temperature down to 4.2 K showing no anomalies correspoinding to phase transitions. On the other hand, the dielectric constants of K
3D(SO
4)
2 and Rb
3D(SO
4)
2 show λ-type anomalies at 84 K and 71 K, respectively. The results indicate that the deuteration in these compounds promotes phase transitions in low temperature region.
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Mamoru Tanibayashi
1980 Volume 48 Issue 3 Pages
890-897
Published: March 15, 1980
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Polarization of NaCl crystals was measured by vibrating it as a cantilever. From the wave form of the potential difference caused by polarization, a new model of dislocation motion was proposed. The changes of the magnitude and the wave form of the induced voltage were interpreted with this model and satisfactory agreements were obtained.
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Kenji Akiyama, Yoshiyuki Morioka, Ichiro Nakagawa
1980 Volume 48 Issue 3 Pages
898-905
Published: March 15, 1980
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Polarized Raman and infrared reflection spectra of KNO
3 crystals have been measured at room temperature. Raman and infrared transmission spectra of the high temperature phase of KNO
3 have been also measured. The frequencies of the transverse (TO) and longitudinal (LO) modes of the infrared active vibrations of the crystal have been obtained from the observed reflectivities. The lattice dynamical analysis of the optical active vibrations of the room temperature phase of KNO
3 has been made based on a rigid ion model which includes effective ionic charges and short-range repulsive force constants. Short-range force constants for the non-bonded metal-oxygen and oxygen-oxygen interactions have been determined by the least squares method using the observed Raman frequencies.
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Katsutoshi Aoki, Osamu Shimomura, Shigeru Minomura, Naoki Koshizuka, T ...
1980 Volume 48 Issue 3 Pages
906-911
Published: March 15, 1980
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The first-order Raman spectra of trigonal Se and Te have been measured under pressure up to the semiconductor-metal transition points at room temperature. In both materials, a prominent pressure effect is found as an anomalous shift of the
A1 mode to low frequency. This softening indicates interference of the interchain bonding with the intrachain covalent bond. Frequency shifts with pressure show deviations from the lattice dynamical homology of Se and Te. The results are interpreted as aspects of the transition to the puckered layer structure of the high-pressure monoclinic phase of Te.
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Mitsuo Kataoka, Yasuo Endoh
1980 Volume 48 Issue 3 Pages
912-921
Published: March 15, 1980
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In order to elucidate the properties of the cooperative Jahn-Teller effect, the diffuse scattering above the transition temperature has been studied both theoretically and experimentally. The correlations between the triply and the doubly degenerate electronic states interacting with each other via lattice vibrations are discussed on the basis of the static Jahn-Teller effect. Satisfactory explanations are given for both the X-ray experiments on NiCr
2O
4 made by Terauchi
et al. and our neutron experiments on Fe
2TiO
4 where Ni
2+ and Fe
2+ in the tetrahedral sites have electronic ground orbitals of triplet and doublet respectively. The role of vibrational optic modes in the electronic interaction and the applicability of the static Jahn-Teller effect are discussed.
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Kazuyoshi Yamada, Yasuo Endoh, Yoshikazu Ishikawa, Noboru Watanabe
1980 Volume 48 Issue 3 Pages
922-929
Published: March 15, 1980
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The structures of Ge rich amorphous Fe–Ge and Ni–Ge alloys were studied by pulsed neutron total scattering. The partial structure factors of S
GeGe(
Q), S
NiGe(
Q) and S
NiNi(
Q) were determined successfully by using Ni
60 isotope for the Ni–Ge alloys. The Ge atoms in the 10 at% Ni–Ge amorphous alloy were found to construct a similar atomic structure as that of the amorphous Ge, while the intermediate short range order configuration between the tetrahedral random network (TRN) and the dense random packing (DRP) structure was found for the 30 at% Ni–Ge alloy. The Ge–Ge pair correlation for this intermediate short range order could well be reproduced by the modified Ge II microcrystalline model.
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Yoshiyuki Kai
1980 Volume 48 Issue 3 Pages
930-938
Published: March 15, 1980
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The binding of NAD, NADH and ADPR to LADH was accompanied by different temperature dependence of the phosphorescence decay rate of the tryptophan residue buried within the protein over the temperature range 0 to 30°C in aqueous solution. As a result of thermally induced transition with a hysteresis cycle in the response to temperature, the Arrhenius curves of the phosphorescence decay rate for NAD– and ADPR–EtOH–LADH complexes were overlapped with those for NADH– and ADPR–LADH complexes, respectively. The typical value of the decay rate at 0°C for the samples distributed at intervals over the range 20–1.5 sec
−1 suggesting that the degree of stability of LADH dimer decreased in the order NADH–>NAD–>EtOH–>ADPR–LADH. In order to explain those results by thermal fluctuation process, a model for the conformation changes of the micro-environment around the residue is presented.
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Katsuyuki Nakano, Tohru Sugimoto, Hideo Suzuki
1980 Volume 48 Issue 3 Pages
939-942
Published: March 15, 1980
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The absorption spectrum of 3-methyl lumiflavin in solution is reexamined by our previous formulation for π-electron systems, improving the previous estimation of the ratio of oscillator strength of the second to the first absorption band. It is found that the following two screenings are necessary to reproduce the absorption spectrum in benzene: (1) the screening of two-center Coulomb repulsion integrals for all the pairs of atoms except bonded ones; (2) that of the effective nuclear charges
Z′ determined by Julg’s method for Slater-type 2
pz-orbitals. It is also found that the absorption spectrum in ethanol or water can be explained by the model of 3-methyl lumiflavin interacting with two point-dipoles. The angle between the transition moments of the first and second bands is found to be at most 44.4° in benzene, 44.3° in ethanol and 45.8° in water.
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Akio Itoh, Masatoshi Asari, Fumio Fukuzawa
1980 Volume 48 Issue 3 Pages
943-950
Published: March 15, 1980
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The single and double electron capture cross sections σ
10, σ
21 and σ
20 of heliumions have been measured in target gases of H
2, He, N
2, O
2, CO
2, CH
4, C
2H
6 and C
3H
8 in the energy range from 0.7 to 2.0 MeV. The measured cross sections are compared with other experimental and theoretical values for the target gases of H
2, He, N
2 and O
2. The additive rule for the charge-changing process of helium ions has been verified by using the cross sections for the carbon-containing molecules. Capture cross sections of helium ions in the collisions with carbon atoms have been estimated.
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Keiichi Tanaka, Setsuo Akiyama, Taso Ikeura, Eizi Hirota
1980 Volume 48 Issue 3 Pages
951-957
Published: March 15, 1980
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The transverse relaxation time
T2 was measured for inversion doublets of the NH
3 molecule from free induction decay signals. The results on the five J=K levels and the nine J=K+1 levels agreed satisfactorily with the values from linewidth experiments. The observed free induction decay signals were also analyzed by a Fourier transformation.
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Kenji Ebihara
1980 Volume 48 Issue 3 Pages
958-964
Published: March 15, 1980
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In order to estimate radial electromagnetic energy flow directed toward a tube axis and plasma heating power for theta pinch discharges, experimental measurements with probes were performed. Time development for the spatial distributions of the electromagnetic energy flow and the plasma heating power density was obtained, so that some interesting phenomena of the theta pinch plasmas were revealed; that is, at the compression phase, the radial distribution of the Poynting vector has a hump under special discharge conditions and total plasma heating power shows a maximum at earlier time than the total electromagnetic input power does.
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Takashi Maekawa, Yasushi Terumichi, Shigetoshi Tanaka
1980 Volume 48 Issue 3 Pages
965-972
Published: March 15, 1980
Released on J-STAGE: June 01, 2007
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Incident lower hybrid waves propagate toward the center of the plasma in a spiral form in the poloidal and the toroidal sections and finally are absorbed by the ion and/or the electron Landau damping within the limited spatial region in accordance with the refractive index parallel to the magnetic field,
N⁄⁄, which is varied considerably along the trajectory, because of the toroidicity and the rotational transform. We propose the scaling law of the wave trajectories on plasma parameters, which shows that the control of
N⁄⁄ or the applied frequency is necessary during the lower hybrid heating. These wave trajectories and damping based on the unmagnetized ion model are compared with those based on the magnetized ion model.
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Sanae Inoue, Kimitaka Itoh, Shoichi Yoshikawa
1980 Volume 48 Issue 3 Pages
973-982
Published: March 15, 1980
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Kinetic theory of low frequency instabilities of a current-carrying finite-β plasma in a sheared magnetic field is investigated. Drift mode, drift-Alfvén mode and drift-tearing mode are identified both in collisionless and collisional regimes and each critical stability condition is obtained, We find a new electromagnetic localized mode driven by the plasma current in a finite-β plasma. Both the current and finite-β effects are required to excite this mode. It is also shown that, in the absence of the plasma current, any electromagnetic localized mode which is propagating in the direction of the electron diamagnetic drift is stable in the collisionless limit of a finite ion temperature plasma. For the collisional mode, stability holds if ω>ω
* (electron diamagnetic frequency) or ω<0.
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Masao Sugawa, Reiji Sugaya, Hisayuki Nomoto
1980 Volume 48 Issue 3 Pages
983-992
Published: March 15, 1980
Released on J-STAGE: May 29, 2007
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Two modes of electrostatic ion cyclotron waves excited in an ion beam plasma system are observed. One of these modes has a sharp and strong spectrum and its dispersion characteristics coincides with one of the backward electrostatic ion cyclotron wave with respect to the propagating component parallel to the magnetic field, the other has a broad spectrum and its dispersion characteristics coincides with one of the forward electrostatic ion cyclotron wave. These excited backward and forward waves occur due to the absolute and convective instabilities. And the transition between two instabilities is observed depending on system parameters. Also, the experimentally obtained temporal and spatial growth of these instabilities are compared with the theory of the weak beam approximation.
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Kazuhiro Nozaki, Katsunobu Nishihara
1980 Volume 48 Issue 3 Pages
993-997
Published: March 15, 1980
Released on J-STAGE: June 01, 2007
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It is shown that deflagration waves supported by thermal radiation are classified into two types, a supercritical and a subcritical deflagration. Their characteristics and structures are investigated in the framework of the diffusion approximation for radiation flux. The subcritical deflagration is found to be easily obtained and to lead to larger compression than the supercritical. The efficiency of compression driven by the deflagration waves is estimated to be 0.1∼0.3.
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Shinichiro Yanase
1980 Volume 48 Issue 3 Pages
998-1008
Published: March 15, 1980
Released on J-STAGE: June 01, 2007
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The stability of natural convection in a fluid layer between co-axial cylinders is investigated theoretically. Temperatures of the two cylinders are different by 2
T0 and a uniform temperature gradient β(<0) is present in the vertical direction, and the ratio of the radii of the outer and inner cylinders is changed from 0 to 1. It is found that there exist three distinguishable instability modes and according to the values of
T0, β and the ratio of the radii, one of the three modes becomes unstable.
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Shigeki Morioka
1980 Volume 48 Issue 3 Pages
1009-1017
Published: March 15, 1980
Released on J-STAGE: June 01, 2007
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A steady, two-dimensional jet-flow of a dispersive compressible fluid issuing a medium at rest is considered on the basis of the linearized theory. The explicit solution is presented by using the Fourier transform technique and by solving the associated dual integral equations. The supersonic jet-flow shows almost periodic oscillation and exponential damping, while the regular subsonic jet-flow is permitted only for uniform stream with constant cross-section. Both solutions are reasonably connected at the critical upstream condition and they are also reduced to the solutions in ordinary gasdynamics as the dispersion vanishes.
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Hirohumi Tougou
1980 Volume 48 Issue 3 Pages
1018-1023
Published: March 15, 1980
Released on J-STAGE: June 01, 2007
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This paper considers the roll-wave phenomenon out shallow turbulent flow down an inclined open channel. On the assumptions of long wave lengths and the Chézy formula for bottom resistance, Dressler has obtained periodic permanent roll-wave solutions with discontinuous water jumps. There exists a one-parameter family of possible wave trains for prescribed average discharge rate. However, if unstable wave trains are contained, they will not be realized. The linear stability of the permanent roll-wave train is then investigated to examine what wave trains are unstable in the family. They are shown to be unstable if their wave lengths are shorter than a certain critical value.
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Yoshimasa Matsuno
1980 Volume 48 Issue 3 Pages
1024-1028
Published: March 15, 1980
Released on J-STAGE: June 01, 2007
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Exact N-soliton and N-periodic wave solutions of the higher order Benjamin-Ono (B–O) equation
ut=−(∂⁄∂
x)(δ
In⁄δ
u) are presented for
n=5 by using bilinear transformation method, where
In is the
n-th conserved quantity of the B–O equation and δ⁄δ
u denotes the functional derivative. For
n≥6, a method for transforming the higher order equations into the bilinear forms is proposed and explicit N-soliton solutions are speculated.
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Kazuhiro Fukushima, Miki Wadati, Takeyasu Kotera, Katsuro Sawada, Yosh ...
1980 Volume 48 Issue 3 Pages
1029-1035
Published: March 15, 1980
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The recurrence phenomena in nonlinear transmission line are studied quantitatively. For various frequencies and amplitudes of the input sinusoidal wave, the recurrence length is measured. The experimental results are explained by a simple theory which assumes the velocity differences of solitons cause the recurrence phenomena.
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Takashi Sakuma, Sadao Hoshino
1980 Volume 48 Issue 3 Pages
1036
Published: March 15, 1980
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Hajime Takayama
1980 Volume 48 Issue 3 Pages
1037-1038
Published: March 15, 1980
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The commensurate(C)-incommensurate(IC) transition in a 2D classical sine-Gordon (SG) system is examined by analyzing the soliton creation energy
ES of the 1D quantum SG system which is derived from the original 2D problem. The C–IC transition point, specified by the condition
ES=0, depends explicitly on the cutoff parameter appearing in the 1D quantum problem.
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Kazuyuki Itoh, Teruto Kataoka, Hironori Matsunaga, Eiji Nakamura
1980 Volume 48 Issue 3 Pages
1039-1040
Published: March 15, 1980
Released on J-STAGE: May 29, 2007
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Distribution of the X-ray Bragg reflections in the reciprocal space was investigated for K
2ZnCl
4 at room temperature by means of the Weissenberg method. The structure in the ferroelectric phase is interpreted as a modulated structure, with a tripled
c-axis of the unmodulated high-temperature structure, induced predominantly by a transverse phase modulation polarized along the ferroelectric
a-axis. The atomic displacements due to the modulated waves are estimated from the crystal structure determined by Mikhail and Peters.
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Hikaru Terauchi, Taiji Kohigashi, Takashi Ohga, Masaru Kawaminami, Tos ...
1980 Volume 48 Issue 3 Pages
1041-1042
Published: March 15, 1980
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The X-ray scattering profiles from WO
3 single crystal are carefully examined to investigate the acoustic instability near the monoclinic-orthorhombic phase transition temperature
Tc=310°C. The spontaneous shear strain
ezx is 0.016 at 25°C, decreases with increasing temperature and becomes zero at
Tc. The temperature dependence of X-ray diffuse scattering intensity indicates that the elastic stiffness consant
C55 becomes vanishingly small just above
Tc.
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H. W. Graben, Kai-Ning Chang
1980 Volume 48 Issue 3 Pages
1043-1044
Published: March 15, 1980
Released on J-STAGE: May 29, 2007
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The Rayleigh-Ritz variational principle is used to formulate a rigorous bound on the threshold conditions under which three helium four atoms will form a bound state when their pair interaction is represented by the Lennard-Jones (n, 6) model and their nonadditive interaction is taken to be the Muto-Axilrod-Teller triple-dipole potential. The accepted parameter values of the model with n equal to 12 predict a bound-state trimer. The oversight, that of failing to use the (12, 6) parameter values of Kihara, Midzuno and Shizume in the extensive work on liquid helium, is pointed out.
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