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Toshiyuki Toyoda
1964 Volume 19 Issue 10 Pages
1757-1758
Published: October 05, 1964
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In order to obtain some physical concept of the conventional symmetry problems of fundamental interactions a new interpretation of the infinitesimal generators of the special unitary group SU(
n) is proposed. A mathematical equivalence between the generators and the permutation operators of two states including sign-change operators is proved. An application of this method to SU(4) is given.
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Masato Morita, Reiko Morita
1964 Volume 19 Issue 10 Pages
1759-1764
Published: October 05, 1964
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Induced effects in muon capture reactions are investigated under the assumption of possible
G-parity nonconservation. The explicit formula of the partial transition rate is given for each forbiddenness in the formalism introduced by Morita and Fujii.
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Hironari Miyazawa
1964 Volume 19 Issue 10 Pages
1764-1768
Published: October 05, 1964
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Behavior of pions in nuclear matter is different from that of free pions due to strong interactions with nuclear-particles. The modified pion propagator and pion-nucleon coupling are calculated in this paper with the static approximation for nucleons. It is expected that the pion mass is decreased in the nucleus by about 15 Mev and the coupling constant is increased by 15 percent. Implication of these results is discussed.
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Akito Arima, Hideo Kawarada
1964 Volume 19 Issue 10 Pages
1768-1782
Published: October 05, 1964
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The seniority scheme introduced by Racah is generalized in the case of degenerate levels. Many formulae for the pure configuration
jn are modified in order to calculate matrix elements in this generalized seniority scheme. It is especially the most interesting result that the diagonal matrix element of two-body operators between the states with the same seniority
v can be expressed in terms of the matrix elements in the
v-particle system. This result, of course, holds in the case of the pure configuration.
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Hisashi Horie
1964 Volume 19 Issue 10 Pages
1783-1799
Published: October 05, 1964
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The fractional parentage coefficients are treated by using the Young operator of the symmetric group and general expressions for the coefficients are obtained. From these expressions one can evaluate the fractional parentage coefficients which separate any numbers of particles from the others for pure or mixed configurations. In order to calculate the fractional parentage coefficients which split off more than one particles, non-standard representations of the symmetric group are made use of. The representations are the outer products of two representations of the symmetric group and the transformation coefficients with the standard representations are calculated.
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Seiji Kabe, Sadayuki Kato, Tadashi Kifune, Yoshitaka Kimura, Masaaki K ...
1964 Volume 19 Issue 10 Pages
1800-1808
Published: October 05, 1964
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Positive pions with energies ranging from 30 MeV to 150 MeV were produced on a carbon target by the bremsstrahlung beam from the 750-MeV electron-synchrotron and detected by means of a π-μ decay counter telescope at an angle of 90° in the laboratory. The counts were corrected for the electronic efficiency of the pion counting system and for the loss of pions in the detection system by decay in flight, nuclear absorption, nuclear scattering and multiple Coulomb scattering. Absolute cross sections of the pion production are given as a function of the peak bremsstrahlung energies extending from 180 MeV to 550 MeV. Applying the photon difference method to the cross section per equivalent quantum, the differential cross sections, (
d2σ⁄
dΩdTπ) and (
dσ⁄
dΩ), are obtained, and compared with theoretical values, which are calculated on the bases of the impulse and closure approximation, the nuclear momentum distribution of a Gaussian type of the average kinetic energy of 19 MeV, and the optical model treatment of the final pion-nucleus interactions. Fair agreements between the experiment and the theory are obtained, and the results support the assumption of the initial production of pions throughout the nuclear volume. A remarkable 3-3 resonance effect is also found in the case of the bound nucleon, and no appreciable nuclear effect other than those due to the nuclear momentum distribution and final state interactions could be observed.
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Shoji Shirato, Shinzou Kubota, Hisao Takahashi, Tadayoshi Doke, Iwao O ...
1964 Volume 19 Issue 10 Pages
1809-1817
Published: October 05, 1964
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Distributions of fragment kinetic energies and masses in the 55 MeV proton-induced fission of U
238 have been measured in various directions with respect to the beam by using a back-to-back arrangement of surface-barrier detectors. The observed energy distribution showed a single broad peak with a slight shoulder on the high energy side. This indicates a marked growth of symmetric fission. The most probable value of the total fragment kinetic energy was observed to be 156±5 MeV. The initial total kinetic energy before neutron emission was estimated from the value to be about 161 MeV. The mass distribution obtained in the transverse direction was in fair agreement with the radiochemical result. By making a fine comparison between these results, an attempt was made to obtain some information about neutron yields from individual fragments. The mass distribution in the backward direction was almost the same in shape as in the transverse direction, when corrected for the projectile momentum. Furthermore, the observed angular distribution of the composite fragments was less anisotropic than expected from the Halpern-Strutinski theory.
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Takuji Yanabu, Sukeaki Yamashita, Shigeru Kakigi, Dai-Ca Nguyen, Kiyoh ...
1964 Volume 19 Issue 10 Pages
1818-1823
Published: October 05, 1964
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The angular distributions have been obtained for alpha-particles from the reactions Be
9 (
p, α) Li
6 (ground state), Be
9 (
d, α) Li
7 (ground, first and second excited states), B
10 (
p, α) Be
7 (ground state), B
10 (
d, α) Be
8 (ground state), B
11 (
p, α) Be
8 (ground state) and B
11 (
d, α) Be
9 (ground and second excited states), and from the elastic and inelastic (second excited state) scatterings of alpha-particles by Be
9. Besides, the angular distribution of deuterons from the reaction Be
9 (
p,
d) Be
8 (ground state) was measured. The energies of incident beams were nearly 7 MeV for protons, 14 MeV for deuterons and 28 MeV for alpha-particles. The results, except for B
10 (
p, α)Be
7 and B
11(
p, α)Be
8, show forward and/or backward rises and may be interpreted by direct interactions. The integrated cross sections of the reactions (
p, α) and (
d, α) on Be
9 are larger than those on B
10 and B
11.
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Kazukiyo Nagata, Muneyuki Date
1964 Volume 19 Issue 10 Pages
1823-1828
Published: October 05, 1964
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A precies experimental study of the paramagnetic resonance line width in CuF
22H
2O was made over a wide temperature range (1.1<
T⁄
TN<30). The result shows that the line width is isotropic at high temperatures but it becomes anisotropic below about 26°K. It was found that the temperature dependence of the paramagnetic resonance line width
ΔH can be expressed by the following empirical formula:
ΔH−[
ΔH]
∞=
A′
T⁄
TN−1)
−n,
where [
ΔH]
∞ is the line width in the high temperature limit.
A and
n are the constants determined as follows:
1.1<
T⁄
TN<1.3
n=1.1±0.1 along both the a and c axes,
A=16±2
Oe(
H\varparallela-axis),
A=25±3
Oe(
H\varparallelc-axis),
1.3<
T⁄
TN<2.0
n=1.9±0.2 along both the a and c axes,
A=6±1
Oe(
H\varparallela-axis),
A=11±1.5
Oe(
H\varparallelc-axis).
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Tatsuo Shimizu, Masatoshi Nakayama
1964 Volume 19 Issue 10 Pages
1829-1836
Published: October 05, 1964
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Spin-lattice relaxation rates through direct, Raman and Orbach processes are calculated for the
MJ=±1⁄2 ground state of shallow acceptors in silicon crystal subjected to a uniaxial stress along the [001] and [111] crystallographic axes. Numerical evaluations are performed using the values of the deformation potential constants recently calculated by the effective mass theory. Effect of f(
q)-factor (
q-th Fourier component of the charge distribution of the acceptor hole) are taken into account to reduce the Raman relaxation rate from
T9-law. Fairly good agreement is obtained between the results of the calculation and preliminary experiment of Ludwig and Woodbury.
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Toshinosuke Muto, Syoiti Kobayasi
1964 Volume 19 Issue 10 Pages
1837-1849
Published: October 05, 1964
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It is well-known that the exchange-polarized core
s-electrons by partially filled magnetic
d-band electrons are able to make characteristic contributions to effective magnetic field felt by nucleus within crystal, which leads to temperature-dependent and negative Knight shift (indirect Knight shift) and nuclear magnetic resonance absorption in ferromagnetic metals. The mentioned exchange-polarization of core
s-electrons has been worked out quantitatively only for the case of isolated atom and ion, and the extension to the crystal electrons in energy band has not been worked as yet mainly for the formidable labour of numerical computations. In view of the above situation we have adopted the perturbation-theoretic approach for working the mentioned problem. The empirical formula of indirect Knight shift by Clogston
et al. and of NMR in ferromagnetic metals by Portis
et al. have been derived successfully and the extension of our formalism to dilute ferromagnetic alloys has been worked.
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Yoshikazu Hamaguchi, Nobuhiko Kunitomi
1964 Volume 19 Issue 10 Pages
1849-1856
Published: October 05, 1964
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The neutron diffraction, electrical resistivity and magnetic susceptibility measurements on b.c.c. Cr-Mn alloys containing manganese from 7.0 to 25.3 atomic percent have shown that the alloys are antiferromagnetic but disordered atomically. The obtained results are shown to be compatible with the theoretical conclusions from the spin density wave model.
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Masao Shimizu, Atsushi Katsuki
1964 Volume 19 Issue 10 Pages
1856-1861
Published: October 05, 1964
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The temperature variations of the electronic specific heats and the magnetic susceptibilities are calculated for Zr and Rh metals by making use of the density of states curves determined from the low temperature specific heat data for 4d-group transition metals and their alloys. The temperature variations of the electronic specific heats of these metals are well explained by the calculated results. The calculated values of the spin paramagnetic susceptibility without a molecular field are considerably smaller than the observed susceptibilities. For Zr metal the difference is mainly attributable to the orbital paramagnetism and its orbital paramagnetic susceptibility is estimated as about 1.0×10
−4 emu/mole. From an analysis of the susceptibility in Rh metal, three possibilities are suggested to explain the experimental temperature variation of susceptibility.
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Masanobu Sakamoto
1964 Volume 19 Issue 10 Pages
1862-1866
Published: October 05, 1964
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The total scattering cross sections of hydrogen atoms for thermal neutrons were measured as a function of the neutron energy for TiH
1.3, TiH
1.6, TiH
1.9, TiH
2.0, VH
0.25, NbH
0.85 and TaH
0.7 at room temperature.
The results clearly show the effect of the inelastic scattering of neutrons, due to excitation of the hydrogen vibrations, and are utilized to determine the energy levels of the optical vibrations in the hydride lattices. They are 0.135 eV for TiH
1.3−2.0, 0.165 eV for VH
0.25, 0.150 eV for NbH
0.85, and 0.145 eV for TaH
0.7.
It was found that there is an approximately linear relation between the energies of the optical phonons and the metal-hydrogen distances reported on various hydrides, except for palladium hydride.
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Hidetaro Abe, Motohiro Matsuura
1964 Volume 19 Issue 10 Pages
1867-1880
Published: October 05, 1964
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Proton NMR in single crystals of Mn(HCOO)
2·2H
2O has been observed at the temperature region from 2.5°K to 300°K. The shift of the resonance lines is explained by a dipole sum carried out by the use of atomic parameters presumed from those of the isomorphous magnesium formate. The results give a good agreement with the experimental data obtained above 4.2°K, if the magnetic moments of two kinds of manganese ions in the crystal are assumed to be
ciH⁄(
T+
Θ) for those of the one kind and to be
ciH⁄
T for the other, where
ci is
g2β
2S(
S+1)⁄3
k,
g=2.00,
S=5⁄2, and
Θ is 9.4±0.7°K.
Since an abrupt shift of the NMR lines occurs at 3.70±0.05°K, a magnetic transition is thought to exist at this temperature. It is presumably due to a sort of magnetic ordering in the one set of ions which is found to have an antiferromagnetic temperature dependence. At this temperature, a change in ESR spectrum and a sharp peak in the susceptibility are also found. Below this temperature, one of the NMR lines has a zero field shift and shows an angular dependence remarkably distorted from a sinusoidal variation.
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Satoru Fujime, Denjiro Watanabe, Shiro Ogawa, Kunio Fujiwara, Shizuo M ...
1964 Volume 19 Issue 10 Pages
1881-1892
Published: October 05, 1964
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In order to elucidate the origin of satellite reflections flanking the direct spot in the electron diffraction pattern of a single crystal evaporated film with CuAu II type superlattice. the peak as well as integrated intensities have been measured as functions of the wavelength of electrons corresponding to the accelerating voltage from 75 to 280 KV. It has been revealed that the intensity of the satellite in question relative to a fundamental reflection consists of two parts, a major part which depends on the wavelength in such a way as predicted by the theory of multiple reflection, and the other minor part which is independent of the wavelength. The existence of the latter part shows that the reflection is not a forbidden one and, therefore, a lattice modulation accompanies the regular anti-phase structure. Fourier potential due to this lattice modulation,
Vs, is estimated to be in the order of one tenth the magnitude of
V400. Some consideration concerning the nature of the modulation is given by comparing the results of electron and X-ray diffraction studies.
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Katsumichi Yagi, Goro Honjo
1964 Volume 19 Issue 10 Pages
1892-1905
Published: October 05, 1964
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A new method of electron beam flashing for preparing thin single crystal films of non-conducting substances has been developed. With use of the method, mechanically introduced and grown-in dislocations and precipitates in NaCl containing 0.00 to 2.3 mole % of CaCl
2 are observed by transmission electron microscopy. The Burgers vectors of dislocations are determined by observing their contrast change which occurs when the crystal is set for different Bragg reflections. Characteristic climb of them into helical form due to electron irradiation is observed. The rate of climb expressed by the number of vacancy pairs causing climb per incident electron of 100–150 keV is found to be of the order of 10
−5 in the films of NaCl containing 0.1 mole % of CaCl
2 about 5000Å in thickness. Observations on incipient and final precipitates in NaCl containing more than 0.3 mole % of CaCl
2 are compared with the results of previous X-ray studies.
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B. N. Misra
1964 Volume 19 Issue 10 Pages
1906-1908
Published: October 05, 1964
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The electron spin resonance absorption study of Picryl-N-amino carbazyl (PAC) in benzene and chloroform solutions at five different dilutions have been made at 9.5 Kmc. At higher dilutions, well separated by hyperfine components have been observed. The measurements of line width of each hyperfine lines, separations between the lines and
g values have been made. A good fit between theoretically computed and experimentally observed absorption spectra have been found by assuming that hyperfine lines have equal width, are equally separated and have Lorentzian shape.
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Minoru Sugawara, Yoshisuke Hatta
1964 Volume 19 Issue 10 Pages
1908-1914
Published: October 05, 1964
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Langmuir probe characteristics for a plasma having oscillations of space potential, electron density and electron temperature are discussed in detail. The method to derive amplitudes of oscillation as well as values of d.c. component of them in the case of the ideal plane probe are introduced.
In order to get informations about oscillating components, “method of constant current probe” developed by Barnes and Eros is applied with some extention. The newly developed method to determine the amplitude of oscillation of the electron temperature seems to be useful because of its improved accuracy.
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Toshihiko Dote, Hiroshi Amemiya
1964 Volume 19 Issue 10 Pages
1915-1924
Published: October 05, 1964
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A magnetic field, impairing the transverse motion of electrons across it, causes a negative current-voltage characteristic to a cylindrical probe whose axis is along the field. This occurs above a certain magnetic field at a low pressure range in neon, argon, krypton, and mercury plasmas. The analysis of this phenomenon is made by using the orbital motion theory inside the sheath. The maximum point in this characteristic is proved to be the space potential. The conventional method for determining the number of concentration of charge particles from this point, however, is no longer valid. The positive ion saturation current is shown to remain useful below 3.3
A1⁄2 kilogauss, where
A is the atomic mass number of ions.
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Seiji Ohara
1964 Volume 19 Issue 10 Pages
1925-1933
Published: October 05, 1964
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The anode current-voltage characteristics of inert-gas-filed triodes have shown current maxima at applied anode voltages corresponding to the first excited potentials of the ambient gases. With increasing gas pressure the current peaks become remarkable. These phenomena are peculiar to heavy rare gases such as xenon and krypton and are not observed in argon, neon or helium. By using this negative resistance as a circuit element, experiments on oscillation are made and the maximum frequencies obtained was 50 Mc/s. The current peak disappears when a few percent gas of diatomic molecules are mixed in the main gases. It is proposed that this unusual electronic conduction through neutral-rare gases is due to an anomaly concerning the scattering process between electrons and metastable atoms similar to the Ramsauer effect.
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Amar Nath Nigam
1964 Volume 19 Issue 10 Pages
1933-1935
Published: October 05, 1964
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From the data on
Kα satellite lines, the values of the corresponding screening constants have been calculated. It is shown that for transitions with the same final and initial electronic configuration but different levels the values of the screening constants are widely different. Some values are negative. It is proposed that a triply ionised X-Ray state can be responsible for one of the negative values of the screening.
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Naobumi Honda
1964 Volume 19 Issue 10 Pages
1935-1954
Published: October 05, 1964
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A quantum mechanical treatment of relaxation phenomena in high temperature plasmas is developed. For a test particle moving with a momentum in a plasma the transition probability for the scattering to another momentum state due to interactions with plasma particles is calculated exactly. Both the binary and the collective interaction are automatically involved in the calculation which has not been the case in the previous theories. With use of this transition probability relaxation rates with exact numerical factors in the arguments of Coulomb logarithms are obtained. It is also shown that Kihara’s connection formula can be derived in the present scheme. Thus a foundation is laid for the unified theory.
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Hideya Gamo
1964 Volume 19 Issue 10 Pages
1955-1961
Published: October 05, 1964
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The thermodynamic entropy of partially coherent light beams, as shown by M. von Laue, is given by the sum of the entropy of the principal waves, which represent the given light beams and are statistically independent of each other. The principal waves and their intensities are respectively the eigenfunctions and eigenvalues of the mutual intensity, cross-correlation function of waveamplitudes, which is positive semidefinite Hermitian operator. The well-known entropy of thermal radiation is applied to principal waves obtained after appropriate reversible optical transmission.
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T. K. Chaudhury
1964 Volume 19 Issue 10 Pages
1961-1965
Published: October 05, 1964
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In this paper the motion of viscous liquid in a curved pipe bent in the form of a circle is discussed. The cross-section of the pipe is of the form
r=
f(θ) having a line of symmetry and the dimension of the section is assumed to be small compared to the radius of the circle traced out by a point within the section. The line of symmetry of the section is taken in the plane of curvature of the pipe in one case and perpendicular to the plane of curvature in the other case. A method of Fourier expansion is applied to find an approximate main flow velocity in the pipe by assuming a uniform stream as the secondary flow in the plane of cross-section. Particular case for a curved pipe of elliptic section of eccentricity 0.25 is worked out.
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Tomomasa Tatsumi, Kanefusa Gotoh, Kyôzô Ayukawa
1964 Volume 19 Issue 10 Pages
1966-1980
Published: October 05, 1964
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The stability of a free boundary layer between two uniform streams is investigated at large Reynolds numbers.
The amplification rate of the disturbances is calculated for all ranges of the wave-number. The critical wave-number does not change appreciably at Reynolds numbers larger than 10
3, and the damping disturbance still exists in the limit of infinite Reynolds number or vanishing viscosity.
The amplitude function of the disturbance is also calculated for various values of the wave-number at infinite Reynolds number. The function has Hermitian symmetry and becomes more concentrated to the origin as the wave-number increases.
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Kazuo Gesi, Yukio Kazumata
1964 Volume 19 Issue 10 Pages
1981
Published: October 05, 1964
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Masao Tomura, Toshio Masuoka, Hitoshi Nishimura
1964 Volume 19 Issue 10 Pages
1982
Published: October 05, 1964
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Hiroshi Suzuki, Noriyoshi Sato, Yoshisuke Hatta
1964 Volume 19 Issue 10 Pages
1983
Published: October 05, 1964
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Kunisuke Asayama, Masaaki Kontani, Junkichi Itoh
1964 Volume 19 Issue 10 Pages
1984
Published: October 05, 1964
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Mituo Ono, Shunkiti Hirokawa, Hideo Nagai
1964 Volume 19 Issue 10 Pages
1985
Published: October 05, 1964
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Hiroshi Ikushima, Shigeru Hayakawa
1964 Volume 19 Issue 10 Pages
1986
Published: October 05, 1964
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Mutsuo Ohta, Fumio Hashimoto
1964 Volume 19 Issue 10 Pages
1987
Published: October 05, 1964
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Hisao Katsuraki
1964 Volume 19 Issue 10 Pages
1988
Published: October 05, 1964
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Ichiroh Nakada, Takahiro Kojima
1964 Volume 19 Issue 10 Pages
1989
Published: October 05, 1964
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Shigeru Hayakawa, Kiyotaka Wasa
1964 Volume 19 Issue 10 Pages
1990
Published: October 05, 1964
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Masao Tomura, Kazuo Murase, Masamine Takebayashi, Tadayoshi Kitada
1964 Volume 19 Issue 10 Pages
1991
Published: October 05, 1964
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Yoshisuke Hatta, Tohru Itoh, Shigeru Handa, Kunihiko Shirahata
1964 Volume 19 Issue 10 Pages
1992
Published: October 05, 1964
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Yasushi Terumichi, Toshitaka Idehara, Isao Takahashi, Hiroshi Kubo, Ke ...
1964 Volume 19 Issue 10 Pages
1993-1994
Published: October 05, 1964
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Jerome I. Kaplan
1964 Volume 19 Issue 10 Pages
1994
Published: October 05, 1964
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Takeki Iwashita, Takashi Inamura, Seizaburo Kageyama
1964 Volume 19 Issue 10 Pages
1995-1996
Published: October 05, 1964
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Hiroji Ohigashi, Ichimin Shirotani, Hiroo Inokuchi, Shigeru Minomura
1964 Volume 19 Issue 10 Pages
1996-1997
Published: October 05, 1964
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Takaaki Hanyu
1964 Volume 19 Issue 10 Pages
1997A
Published: October 05, 1964
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One of the photographs in the paper entitled as above (Fig. 1 (b)) was misprinted and should be corrected to rotate about the axis perpendicular to the paper by 1800.
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Eizo Otsuka, Seiichi Nagata, Kazuo Murase, Hiroo Yonemitsu
1964 Volume 19 Issue 10 Pages
1997B
Published: October 05, 1964
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Eizo Otsuka, Seiichi Nagata, Kazuo Murase, Hazimu Kawamura
1964 Volume 19 Issue 10 Pages
1997C
Published: October 05, 1964
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Table I in the first paper and Table I in the Second Paper Should be Interchanged.
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