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Yukichi Yamaguchi, Jian-zhi Runan(Gen), Teruaki Nagahara
1975 Volume 38 Issue 4 Pages
911-916
Published: April 15, 1975
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The gamma-ray spectrum and the conversion-electron spectrum are measured in the decay of the
116mIn activity. Directional correlations are also measured for 818–1293 and 1097–1293 keV cascades. The M1-E2 mixing ratio δ, and the E0-E2 mixing ratio μ
k are obtained for 818.7 keV 2
2+→2
1+ transition to be δ=1.52
−0.22+0.26, and μ
k≤6.1×10
−4 respectively. The E2 branching ratio
B(E2; 2
2+→0
g+):
B(E2; 2
2+→2
1+):
B(E2; 2
2+→0
1+) is determined to be 0.0158:1.0:5.86.
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Masaaki Kanbe, Manabu Fujioka, Kazuo Hisatake
1975 Volume 38 Issue 4 Pages
917-927
Published: April 15, 1975
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Internal conversion electrons and γ-rays following the decay of
206Po were measured with a π\sqrt2 iron-free β spectrometer and Ge(Li) detectors. The energies and intensities of 80 transitions including 60 new ones have been determined. Especially, we identified a new intense M1 transition of 10.84 keV. The multipolarities for 64 transitions were determined from
K-conversion coefficients and
L- and
M-subshell ratios. γ-γ coincidences employing two Ge(Li) detectors were also performed.
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Masaaki Kanbe, Manabu Fujioka, Kazuo Hisatake
1975 Volume 38 Issue 4 Pages
928-935
Published: April 15, 1975
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Using the results of our conversion-electron and γ-ray measurements in the decay of
206Po, a decay scheme of
206Po is proposed as follows: 0[6
+], 59.91[4
+], 70.76[3
+], 82.83[5
+], 200.40[4
+], 352.71[(4, 3)
+], 409.19[2
+], 523.23[3
+], 733.93[3
+], 878.12[2
+], 897.10[3
+], 931.70[1
+], 1077.89[2
+], 1103.02 [2
+], 1264.77[(2, 3, 4)
+], 1389.45[1
+], 1523.67[1
+], 1567.57[1
+(2
+)] and 1600.14 keV [0
+(1
+)]. In the present decay scheme the previous discrepancy between spin-parities and log
ft values has been removed. The low-lying states in
206Bi are interpreted in terms of one-proton, three-neutron-hole configurations outside the doubly closed
208Pb core.
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Shuzo Uehara
1975 Volume 38 Issue 4 Pages
936-944
Published: April 15, 1975
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Levels of
60Co were studied with 6.5 MeV deuterons
via the
59Co(d, p) reactions with 18 keV resolution. A total of 75 excited levels were identified up to an excitation energy of 5 MeV. The ground state
Q-value was found to be 5.274±0.007 MeV. Angular distributions of each proton groups were measured over the range 25°≤θ≤140°. Then the
ln values were determined and the spectroscopic factors were extracted from comparison with the zero-range DWBA calculations. A sum rule analysis was made for the 2p
3⁄2, 1f
5⁄2 and 2p
1⁄2 single particle states and
Jπ assignments were made for low-lying levels by comparing with the (n, γ) reaction data.
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Isao Kohno
1975 Volume 38 Issue 4 Pages
945-953
Published: April 15, 1975
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Elastic and inelastic scatterings of
14N and
12C particles by
12C and
28Si at energies from 65 to 88 MeV have been studied. Angular distributions of these elastic scatterings were measured over a laboratory angular range from 7 to 35 degrees at intervals of 1 or 1.5 degrees. These angular distributions were analyzed with an optical model, and the scattering amplitudes of all partial waves were obtained.
Angular distributions of inelastic scattering exciting the 2+ and 3− states of
12C and
28Si were measured for
12C+
14N,
12C+
12C and
28Si+
12C, and Mutual excitation of the 2+ states of
12C in
12C+
12C and excitation of projectile
12C in
28Si+
12C were also observed. These angular distributions were analyzed with DWBA using optical parameters fitted to the elastic scattering data. The deformation parameters of
12C obtained were consistent with the values previously reported, but those of
28Si obtained by the analyses were not consistent with ones previously reported.
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Tadao Ishii
1975 Volume 38 Issue 4 Pages
954-964
Published: April 15, 1975
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A bare-ion Larmor frequency in an applied magnetic field is usually washed out by the electron screening effect to result in an elementary excitation, “
phonon·
Alfvon”, while only in the “
ultraintense” field whose energy density is of the order of Fermi energy do we have a new excitation, “
charged phonon”, besides the phonon·Alfvon.
The charged phonons appear at the threshold field
Hth determined nearly by
Hth2⁄8π=ρ
vs2⁄2 where
vs is the sound velocity and ρ is the mass density. The Alfvon part predominates the phonon part for the fields stronger than
Hth (“
phonon-vanishing effect”). The threshold field for these phenomena turns out 0.378 MOe for potassium.
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Takemitsu Hasegawa, Masao Shimizu
1975 Volume 38 Issue 4 Pages
965-973
Published: April 15, 1975
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The approximation method developed by Singwi
et al. for classical distribution function is applied to the Wigner distribution function in a quantum system. In this way a quantum mechanical expression is derived for dielectric function of an interacting electron gas. Self-consistent numerical calculations of structure factor and dielectric function are carried out for an electron gas at metallic density of electrons. Pair distribution function, compressibility, correlation energy and dispersion relation of plasmons are numerically calculated from the calculated structure factor. The calculated results of the pair distribution function are found to be positive for the entire range of real metallic density of electrons.
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Akio Kotani
1975 Volume 38 Issue 4 Pages
974-980
Published: April 15, 1975
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Self-consistent calculations of the incommensurate sinusoidal spin-density-wave in chromium and its alloys are carried out numerically by taking account of a sufficiently large number of Bloch states coupled by the exchange potential. The commensurate-incommensurate transition is also studied. The results are compared with those calculated by two less exact methods proposed in our previous papers. A discussion is given on the amplitudes of harmonics.
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Tohru Morita, Tsuyoshi Horiguchi, Charles C. Chen
1975 Volume 38 Issue 4 Pages
981-988
Published: April 15, 1975
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Numerical calculations of the electronic density of states and the electric conductivity at zero temperature are reported within the coherent potential approximation for random binary alloys on the bcc lattice. The computations are made with the aid of an efficient procedure of evaluating the lattice Green function. A poor-conductive region is observed around the dip of the electronic density of states, just before the dip develops to a gap, for binary alloys with small minority densities.
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Tsuneya Ando
1975 Volume 38 Issue 4 Pages
989-997
Published: April 15, 1975
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The lineshape is studied in the simplest approximation free from the difficulty of divergence caused by a singular nature of the system. Characteristics of the linewidth are obtained for both short- and long-ranged scatterers. By assuming δ-potential scatterers, the lineshape is calculated explicitly as a function of the applied magnetic field in an
n-channel inversion layer on Si (100) surface. At low temperatures, a Shubnikov-de Hass type oscillation appears in the lineshape. At high temperatures, it disappears and the lineshape becomes asymmetric around the resonance magnetic field.
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Hisao Kitaguchi, Shoichi Nagata, Takashi Watanabe
1975 Volume 38 Issue 4 Pages
998-1002
Published: April 15, 1975
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The magnetic susceptibility and the specific heat of Cu(NH
3)
2·Ni(CN)
4·2C
6H
6 in powder specimen has been measured between 0.2 and 20.4 K. Broad maximums are observed near 3 K in both experimental results, but the information for phase transition to the long range order can not be obtained down to 0.2 K. These results give the behaviour of low dimensional magnetic lattice for this crystal. The susceptibility data is explained as the one dimensional antiferromagnetic spin system with exchange interaction |
J|=2.31 K.
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Yûichi Tazuke, Kazukiyo Nagata
1975 Volume 38 Issue 4 Pages
1003-1010
Published: April 15, 1975
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Temperature and angular variation of EPR line-widths of a one-dimensional Heisenberg antiferromagnet CsMnCl
32H
2O have been measured at K-band frequency above its ordering temperature. A minimum in the angular variation appears at room temperature indicating the dominance of long-time,
q∼0 diffusive modes of torque correlation function. However, the line-shape is Lorentzian because of non-negligible magnitude of interchain interactions. As the temperature is lowered, they broaden and the minimum in their angular variation disappears. These phenomena can be understood when one considers the growth of intrachain spin correlation of wave vector
Q0 and the relative importance of short-time, Gaussian decay modes compared with the
q∼0 modes. Line-widths are calculated within Kubo-Tomita’s framework and Fisher’s classical treatment. Good, quantitative agreement is attained particularly at low temperatures.
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Yuji Yamaguchi, Toshiaki Sakuraba
1975 Volume 38 Issue 4 Pages
1011-1019
Published: April 15, 1975
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Magnetization of CsMnF
3 and Ni-doped CsMnF
3 has been measured in the temperature range between 1.6K and 300K and in the magnetic field up to 70 kOe. It has been observed that the susceptibility increases very rapidly with decreasing temperature below
TN and that the susceptibility of Ni-doped CsMnF
3 decreases with increasing magnetic field. This behavior is qualitatively explained from a detailed analysis of the four-sublattice model of molecular field theory. The exchange integrals in CsMnF
3 are evaluated to be
JAB=6.8 K for the 180°-superexchange and
JBB=4.5 K for the 90°-superexchange assuming that all the next-nearest exchange are 0.1 K. The 90°-superexchange between Mn and Ni in Ni-doped CsMnF
3 are estimated to be about −8.5K. With these parameters CsMnF
3 is found to have an antiferromagnetically-coupled ferrimagnetic layer structure.
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Soichi Miyata, Kazuko Motizuki
1975 Volume 38 Issue 4 Pages
1020-1026
Published: April 15, 1975
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Magnetic properties and magnon Raman scattering are studied for a simple cubic antiferromagnet KNiF
3 adopting cluster approximation. The spin states of the cluster consisting of a central spin and its six n. n. spins are solved self-consistently. The Néel temperature, sublattice magnetization, and spin-pair correlation function are calculated. Using the obtained cluster spin states, the temperature variations of the intensity distribution and total intensity are calculated for the Γ
3+ mode over the whole temperature range below and above
TN. Discussion is given for the comparison with observed results.
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Sanchi Mizushima, Yoshiko Fujibayashi
1975 Volume 38 Issue 4 Pages
1027-1031
Published: April 15, 1975
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Current vs voltage relation was measured on graphite at high electric fields under transverse magnetic fields at about 80 K. It was shown that in low mobility specimens the kink appears when the drift velocity of carriers reaches a value which roughly coincides with the velocity of transverse vibrations in the basal plane. On the other hand, in higher mobility crystals the above kink becomes weak, while another kink turns up at higher electric fields, which give as the critical drift velocity a value approximately corresponding to the velocity of in-plane longitudinal vibrations. This dependence of the Esaki effect upon the mobility of the specimen is attributed to the presence of defects which strengthen the interaction between carriers and transverse vibrations of the lattice.
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Hideo Kojima, Takeshi Moriya, Taira Suzuki
1975 Volume 38 Issue 4 Pages
1032-1041
Published: April 15, 1975
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The flow stress change
Δτ associated with superconducting transition has been measured on lead and lead alloy crystals against the kind and the concentration of solute atoms as well as the amount of deformation and temperature.
Δτ increases with applied stress rapidly in the beginning and slowly in later stages of deformation. The temperature dependence of
Δτ cannot simply be expressed as proportional to (1−
Bs⁄
Bn), where
Bn and
Bs are the electronic drag coefficients of a dislocation in normal and superconducting states, respectively.
Δτ of lead alloys is dominantly affected by the size misfit between solute and solvent atoms. As to the solute concentration
c,
Δτ∝
cn, where n is first about 1/2 but increases with deformation. These results are discussed theoretically by taking account of the influence of the electron viscosity on both terms of the activation energy and the attempt frequency in the rate equation describing the thermally activated motion of a dislocation.
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Keiichi Kaneto, Yoshinobu Ido, Katsumi Yoshino, Yoshio Inuishi
1975 Volume 38 Issue 4 Pages
1042-1047
Published: April 15, 1975
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Dependence of the phosphorescence emission of Platinum phthalocyanine single crystals around 971 nm on the magnetic field and on the incident laser intensity are investigated. The energy splitting of the spin sublevels of the lowest excited triplet state is about 8.5 cm
−1 in zero field and about 12.4 cm
−1 in the external magnetic field of 50 kG. The T–T (triplet-triplet) annihilation rate is estimated to be about 1×10
−2 cm
3/sec and the magnetic field dependence of the T–T annihilation reveals that the |0> spin component of the triplet exciton plays the most important role. The temperature dependence of the phosphorescence at the low temperature range is also studied.
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Makoto Morita, Kazuyuki Murata
1975 Volume 38 Issue 4 Pages
1048-1055
Published: April 15, 1975
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The luminescence spectra of methylammonium chrome alum, CH
3NH
3Cr(SO
4)
2 12H
2O (MCrSD), are measured from 4.2 K to 200 K in order to clarify spectroscopic behaviour of Cr
3+ ions in the host ferroelectric crystal. The substantial spectral anomalies of the
R1 line and vibronic bands are observed in the region 15,000∼13,000 cm
−1 at around the Curie point (164 K). In particular, the linewidth of the
R1 line reveals a characteristic broadening which is not simply described in terms of the Raman scattering process. The linewidth analysis gives strong evidence for fluctuation of spontaneous polarization in a relaxation process of Debye type. At around 35 K, the
R1 line shows a unusual intensity maximum. These results could be ascribed to a change of the strength of the hydrogen-bonding, associated with a sulphate-group disorder at low temperatures.
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Shinsuke Miura, Masakazu Marutake, Hiromi Unoki, Hiromoto Uwe, Tunetar ...
1975 Volume 38 Issue 4 Pages
1056-1060
Published: April 15, 1975
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Elastic measurement has been done for single crystals of Sr
1−xBa
xTiO
3 (
x=0, 0.006, 0.012, 0.014) and Sr
0.941Ca
0.059TiO
3 in the temperature range from 4 K to 240 K. The structural phase transition temperature
Ta, where elastic anomaly occurred, was found to decrease with Ba-concentration, while it increased with Ca-concentration. Dielectric constants for the Sr
1−xBa
xTiO
3 system have also been measured with stress-treated crystals.
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Ko Sugihara
1975 Volume 38 Issue 4 Pages
1061-1066
Published: April 15, 1975
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Anisotropic spin-dependent energy δ
0(
E)
σ·
\hatκ(
\hatκ∼
O(
k3),
σ: Pauli matrix), introduced by Rashba and Sheka in their study of the combined resonance in III–V compounds, provides a broadening of the Zeeman level. However, the level broadening is extremely narrowed by frequent scattering of the conduction electrons induced by ionized impurity centers. The present mechanism, together with the spin-flip processes related to the ionized impurity scattering and the LO-phonon exchange, gives a qualitative explanation for the observed ESR line width of the degenerate samples in n-InSb.
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Hideyuki Nakagawa, Koichi Toyoda, Yoshio Nakai
1975 Volume 38 Issue 4 Pages
1067-1072
Published: April 15, 1975
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The optical absorption and luminescence of NaCl–NaBr solid solutions were studied in the whole concentration range at liquid nitrogen temperature. The change of the profile observed in the absorption spectra around 0.2 mole fraction of NaBr content is attributed to the percolation of minority composition in this system. With increasing the concentration of NaBr, the 5.15 eV emission band, which is known to arise from Br
−-dimers, shifts gradually toward the low energy side to reach finally the location of the intrinsic emission band in pure NaBr, whereas the 4.0 eV emission band arising from Br
−-monomers diminishes its intensity and fades out above 0.2 mole fraction of NaBr. This suggests that the relaxed excited state of the Br
−-dimer, not of the Br
−-monomer, in NaCl can be recognized as a proto-type of the self-trapped exciton in the pure NaBr.
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S.K. Kor, N.D. Tripathi
1975 Volume 38 Issue 4 Pages
1073-1075
Published: April 15, 1975
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Second-and third-order elastic constant data have been used to evaluate the acoustic mode Grüneisen parameter 〈γ〉, average Grüneisen constant 〈γ
2〉, non-linearity constant
D for Strontium titanate (SrTiO
3). The attenuation suffered by longitudinal and shear acoustic-wave propagating along 〈100〉 and 〈110〉 directions and shear waves polarized along 〈100〉 and 〈10\bar1〉 directions, due to phonon-viscosity and theermoelastic mechanism have been calculated for SrTiO
3 at 295 K. The phonon viscosity in terms of dislocation drag coefficient along 〈100〉 and 〈110〉 directions is also evaluated.
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Takeo Matsubara
1975 Volume 38 Issue 4 Pages
1076-1079
Published: April 15, 1975
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The α-β-γ transitions observed in CuI are interpreted in terms of anharmonic oscillation of Cu ion. Strong temperature dependence of the Debye-Waller factor and large anomalous entropy are correlated consistently within the proposed anharmonic oscillator model.
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R. Ramji Rao
1975 Volume 38 Issue 4 Pages
1080-1082
Published: April 15, 1975
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The second Grüneisen constant of a number of cubic and uniaxial solids has been evaluated at the room temperature from thermodynamic data using a modified formulation of Basset
et al. A method to calculate the Anderson-Grüneisen parameter of a solid from its pressure derivatives data is described.
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Tomoyuki Hikita, Itaru Tatsuzaki
1975 Volume 38 Issue 4 Pages
1083-1089
Published: April 15, 1975
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The nuclear spin-lattice relaxation time of
23Na in a single crystal of silver sodium dinitrite has been measured as a function of temperature. The inverse of the relaxation time monotonically increases with temperature. The anomalous decrease of the relaxation time near the phase transition temperature as observed in sodium nitrite was not found in this ferroelectric. The temperature dependence of the relaxation time was interpreted as a result of EFG fluctuation at the
23Na site caused by the flipping of the two nearest NO
2− ions. The flipping frequency of the NO
2− ion was evaluated to be lower than the Larmor frequency.
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Shigeya Kuwabara, Tateki Uefuji
1975 Volume 38 Issue 4 Pages
1090-1097
Published: April 15, 1975
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From the observation of energy-filtered thickness fringes in electron microscopic bright-field and dark-field images of thin aluminium single crystal films it is found that (1) the fringe positions and distances are almost the same regardless of the filter potential, and (2) the fringe intensities of no-loss, 7 and 15 eV loss electrons decrease slowly as the thickness increases but those of 3 and 10 eV loss electrons decrease rapidly. These effects are explained by using a
n-slice dynamical theory in which the effect of energy losses is taken into account.
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Akira Takahashi
1975 Volume 38 Issue 4 Pages
1098-1105
Published: April 15, 1975
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The two electron wave function of an OH bond of the water molecule is approximated by a linear combination of the covalent and the ionic type wave functions. The mixing coefficient λ in the gaseous state is determined from the observed dipole moment of the molecule. The proton shift relative to the gaseous state is calculated as a function of λ by a variational method. The values of λ for the water molecules, co-ordinated to Al
+++ in the AlCl
3 aqueous solution or to Mg
++ in the crystal of MgCl
2·6H
2O, are empirically determined from the observed shifts. From these values of λ, and the known values of the component of electric field,
F⁄⁄, along the OH bond of the coordinated water molecule, the bond polarizability is estimated. The assumption of constancy for the value of polarizability leads to the result that the shift depends almost linearly on
F⁄⁄.
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Fujio Shimizu
1975 Volume 38 Issue 4 Pages
1106-1109
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Methylchrolide ν
6 band was studied by laser Stark spectroscopy using 10 μm CO
2 lasers. Resonances of approximately 100 transitions of CH
3Cl
35 ν
6 band were identified. Band constants of ν
6 band were calculated.
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Hideo Suzuki, Tohru Sugimoto, Ken Ishikawa
1975 Volume 38 Issue 4 Pages
1110-1118
Published: April 15, 1975
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On the model for phytochrome chromophore proposed by Crespi
et al., the light-absorbing property is examined using the ZDO approximation of the LCAO-ASMO-SCF-CI theory of π-electrons. All the bond lengths together with the bond angles of the pyrrole rings with cyclic π-system are improved in each stage of the iteration processes for solving MO’s, and a sufficient number of configurations are included in the CI calculation.
The interactions of the model chromophore with a negative point-charge and with a point-dipole are also examined on the basis of the stationary perturbation theory for degenerate states, and it is shown that, among the models so far proposed, only the P
fr-form by Crespi
et al. can reproduce the observed absorption spectra of phytochrome, provided its interaction with the electric field caused by protein moiety is taken into account.
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Hidenobu Hori, Kazuharu Toyokawa, Osamu Wakishima, Muneyuki Date
1975 Volume 38 Issue 4 Pages
1119-1124
Published: April 15, 1975
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A new method of producing high density positive charge carriers in liquid He II was developed by using an immersed hot tungsten filament.The production mechanism and transport properties of the positive carriers were investigated both experimentally and theoretically. It was found that when the applied voltage is reversed in the hot cathode diode an electrical discharge occurs in the gas sheath around the filament and the positive ions are emitted from the discharge plasma into surrounding liquid He II. The estimated carrier density is about 10
10 carriers/cc.
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Toshitaka Idehara, Mitsuyoshi Takeda, Yoshio Ishida
1975 Volume 38 Issue 4 Pages
1125-1132
Published: April 15, 1975
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The Bernstein wave propagating obliquely to the magnetic field is excited by the coaxial probe and is heavily damped by the Landau and/or cyclotron damping with respect to the direction along the field, whose propagation direction may be coincident with that of the maximum value of group velocity (∂ω⁄∂
k). When a rather weak electron beam is injected, the wave is amplified due to the convective instability, whose wave vector
k is determined as follows: the wave number component
k|| paralell to the field satisfies the Cherenkov excitation condition (
k||vb≈ω), and then, the component
k⊥ perpendicular to the field is determined by the dispersion relation
K(ω,
k||,
k⊥)=0. Increasing the intensity of the electron beam above the threshold value, the spontaneous excitation of the wave is observed, which can be explained consistently as the result of the convective instability of thermal noise in plasma.
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Tatsuki Ogino, Susumu Takeda
1975 Volume 38 Issue 4 Pages
1133-1140
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A computer simulation is performed to study two types of the parametric instabilities and their saturation states using a fluid model where the fluid transform and Poisson’s equations are computed by the modified 2 step Lax-Wendroff method.
From the simulation, it is clearly confirmed that the decay instability is excited when the pumping dipole field frequency ω
0 is higher than the plasma cut-off frequency ω
p0, and that the oscillating two stream instability is excited when ω
0 is lower than ω
p0. The resonance conditions for the frequency and wave number are well satisfied, and the simulated growth rate agrees well with the theoretical one. Both the instabilities saturate due to the mode-mode coupling when the wave energy approaches the electron kinetic energy.
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Keishiro Niu, Takashi Yabe, Motoo Hori
1975 Volume 38 Issue 4 Pages
1141-1146
Published: April 15, 1975
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An analysis is given of the instability and breaking up of a gas string or a gas board which has a high relative velocity to a surrounding liquid. This situation is chosen as a theoretical model for representing the gas motion in an experiment which is devised to supply a lot of small gas bubbles in a liquid. The governing equations and the boundary conditions for the gas and liquid motions in linearized forms lead us to a dispersion relation between the growth rate of wave and the wave number. The wave length which gives the maximum growth rate coincides with the average diameter of bubbles observed in the experiment.
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Isamu Nakata
1975 Volume 38 Issue 4 Pages
1147-1154
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Weakly non-linear waves on a plane interface between an inviscid and incompressible liquid layer with uniform thickness and a semi-infinite gas with negligible density in an acceleration field normal to the undisturbed plane interface and directed from the liquid to the gas are investigated in the presence of surface tension. The other surface of the liquid layer is assumed being adjacent to a rigid boundary. By means of the derivative expansion method, a non-linear Schrödinger equation for the complex amplitude of a quasi-monochromatic travelling wave is derived. From the known property of this equation, it is found that wave trains of constant amplitude are modulationally unstable. This suggests a new possibility of the instability of the interface. Applying the same method to the state near the marginal stability, the non-linear cut-off wavenumber is obtained irrespectively of an initial condition.
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Kinzo Hida
1975 Volume 38 Issue 4 Pages
1155-1158
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On the basis of Prigogine’s kinetic theory on a traffic flow, a unique relation between the mean speed and the concentration is proposed. In case of low density traffic, the flow (defined by the concentration times the mean speed) versus the concentration is shown by a family of one-parameter curves, which terminates on the critical curve corresponding to a high density traffic. Some remarks are also given to the logarithmic law by Greenberg.
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Yuko Oshima, Tsutomu Kambe, Saburo Asaka
1975 Volume 38 Issue 4 Pages
1159-1166
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Interaction of two vortex rings is examined by experiments and numerical analysis. Experimental observations are carried out in a water tank using the electrolysis method and it is found that the interaction patterns are classified into three types. Numerical simulations are performed by integrating the Navier-Stokes equation and the results of the experiments and calculations are found in good agreement. The game of the passing through each other does not happen in this region of low Reynolds number.
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Hiroshi Tokunaga, Tomomasa Tatsumi
1975 Volume 38 Issue 4 Pages
1167-1179
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Interaction of two intersecting plane nonlinear waves in a compressible fluid such as shocks, expansion waves, slip flows and contact surfaces are investigated using the reductive perturbation method. It is shown that intersections of waves belonging to different families of characteristics do not alter the nature of the waves but change their amplitudes, phase-velocities and paths, whereas intersections of waves belonging to the same family of characteristics make them either coalesce or absorb each other. It is inferred from these results that the statistical properties of two-dimensional shock turbulence is identical to those of the Burgers turbulence.
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Sinzi Kuwabara, Ryuji Takaki
1975 Volume 38 Issue 4 Pages
1180-1186
Published: April 15, 1975
Released on J-STAGE: June 01, 2007
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Possibility of occurrence of secondary flow in boundary layer around a circular cylinder in rotatory oscillation is studied by means of linear theory. The secondary flow can occur above a certain critical Reynolds number, and the condition of occurrence of the secondary flow is shown by curves in the Reynolds and wave number diagrams with a nondimensional thickness of the boundary layer as a parameter. Satisfactory agreement of the results with experimental ones by Taneda
et al. is obtained.
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Naoyuki Tokuda
1975 Volume 38 Issue 4 Pages
1187-1194
Published: April 15, 1975
Released on J-STAGE: June 01, 2007
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Nature of three dimensional viscous flow near corner formed by the intersection of two quarter-infinite flat plates at various angles has been examined by constructing Stokes slow flow solutions. Specifically viscous flows for intersection angles of π, (3/2)π and 2π have been investigated, which correspond to flows past a semi-infinite flat plate, an external flow past a right angle corner and a quarter-infinite flat plate respectively.
On the basis of the Stokes solutions obtained, various types of singularities arising in the flow field are identified over the complete range of intersection angle 0–2π.
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Mitutosi Kawaguti
1975 Volume 38 Issue 4 Pages
1195-1199
Published: April 15, 1975
Released on J-STAGE: June 01, 2007
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Relating to sheet flow theory for microcirculation in lung, two model flows are studied by numerical method. The flow of a viscous fluid through regularly-spaced cylinders is studied by solving numerically the Navier-Stokes equations. Further, the flow of a viscous fluid between two parallel plates interconnected by regularly-spaced cylinders is studied using Hele-Shaw method. The former flow corresponds to the case where the gap between membranes is wide and the effects can be completely neglected. The latter flow corresponds to the case where the gap between membranes is narrower than the spacing of the cylinders.
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Takuji Kawahara
1975 Volume 38 Issue 4 Pages
1200-1206
Published: April 15, 1975
Released on J-STAGE: June 01, 2007
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An extended form of the derivative-expansion method is applied to the study of nonlinear capillary-gravity waves on a liquid layer of slowly varying depth. Generalized expressions of the nonlinear Schrödinger and the Korteweg-de Vries equations including inhomogeneity effects are derived. The results are discussed briefly in connection with those obtained by Whitham’s technique. It is pointed out that the method is widely applicable to the analysis of asymptotic behaviour of the nonlinear dispersive waves in weakly inhomogeneous media.
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B. Singh, H. W. Taylor
1975 Volume 38 Issue 4 Pages
1207
Published: April 15, 1975
Released on J-STAGE: June 01, 2007
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Kazu Nishigaki
1975 Volume 38 Issue 4 Pages
1208
Published: April 15, 1975
Released on J-STAGE: May 29, 2007
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Yuichi Okuda, Motohiro Matsuura, Taiichiro Haseda
1975 Volume 38 Issue 4 Pages
1209
Published: April 15, 1975
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Jun Takeuchi, Toshio Aoi, Yoshika Masuda
1975 Volume 38 Issue 4 Pages
1210
Published: April 15, 1975
Released on J-STAGE: May 29, 2007
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Hideoki Kadomatsu, Hiroshi Fujiwara, Kazuo Ohishi, Yoshiaki Yamamoto
1975 Volume 38 Issue 4 Pages
1211
Published: April 15, 1975
Released on J-STAGE: May 29, 2007
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Katsunori Iio, Mitsumasa Isobe, Kazukiyo Nagata
1975 Volume 38 Issue 4 Pages
1212
Published: April 15, 1975
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Toshihiko Shigematsu, Shin-ichiro Ohmori, Norihiko Nakanishi, Sukeji K ...
1975 Volume 38 Issue 4 Pages
1213
Published: April 15, 1975
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Yoshihiro Takagi, Yukio Fukuda, Meiro Chiba, Koichi Yamada, Tsuneo Has ...
1975 Volume 38 Issue 4 Pages
1214
Published: April 15, 1975
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Natsuki Mori, Masayuki Hosono, Hajime Ozaki
1975 Volume 38 Issue 4 Pages
1215
Published: April 15, 1975
Released on J-STAGE: May 29, 2007
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