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Motoharu Kimura, Naosi Mutsuro, Yuji Ohnuki, Katsufusa Shoda, Masumi S ...
1959 Volume 14 Issue 4 Pages
387-396
Published: April 05, 1959
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The bremsstrahlung spectra of the 8.5 MeV electrons for the forward direction were measured with a scintillation spectrometer of a sodium iodide crystal 4 in. in diameter and 4 in. in length. Be, Ni and Pt of several thickness were used as the targets. The measured spectra were compared with our semi-empirical calculation. The calculation was based . upon the response function for NaI crystal which was constructed referring to the method developed by NBS group and also to the actual response curve for the monochromatic gammas of 1.12 and 6.14 MeV, instead of using Monte Carlo method which had generally been used in the former researches. The agreement is rather good if we assume Schiff’s formula for the intrinsic bremsstrahlung spectra.
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Yukiyasu Oda, Minoru Takeda, Chuin Hu, Shohei Kato
1959 Volume 14 Issue 4 Pages
396-402
Published: April 05, 1959
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The angular distributions of protons scattered elastically and inelastically by Ne
20 and Ne
22 have been observed at six energies from 4.95 to 5.50 Mev. The shape of angular distribution of inelastically scattered protons varies rapidly with incident energy in boths cases of Ne
20 and Ne
22. An anomaly is found at 5.25 Mev in the reaction Ne
20(
p,
p′)Ne
20(
Q=−1.63 Mev). The elastic scatterings also exhibit the corresponding features. These results suggest that the reaction proceeds mainly through the compound nucleus formation process. The spin and parity of the compound state seem likely to be 5/2(+).
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Taro Kihara
1959 Volume 14 Issue 4 Pages
402-410
Published: April 05, 1959
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An effective interparticle potential, which is a modified Debye-Hückel potential, is introduced and discussed in order to eliminate simultaneous interactions between three particles or more in an ionized gas. For this potential weak-interaction asymptotes of collision cross sections necessary for the theory of irreversible processes are calculated without making further approximations. These cross sections are applied to relaxation between ion and electron temperatures and to the coefficient of viscosity.
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Tadao Kasuya
1959 Volume 14 Issue 4 Pages
410-415
Published: April 05, 1959
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The difference between the electric currents due to the external electric field and the gradient of the chemical potential is discussed based on the general theory of transport coefficients. In the limit of weak magnetic field (h
w<<κ
T, where ω is Larmor frequency, κ Boltzmann constant,
T absolute temperature) and weak collision (h⁄τ<<κ
T, where τ means the relaxation time), Einstein relation is applicable. In the limit of strong magnetic field, the current due to the gradient of the chemical potential exhibits the oscillatory behaviour similar to that of diamagnetism.
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Tadao Kasuya, Kazuo Yamada
1959 Volume 14 Issue 4 Pages
416-435
Published: April 05, 1959
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The electrical and thermal conduction phenomena are discussed by taking account of the effects of Coulomb interaction and Umklapp processes of electron-phonon collisions. The contributions of electron binary collisions through screened short range Coulomb potential to a relaxation. processes are evaluated. The effect to the coupling parameter of electron-phonon interaction is also considered in the range of called Umklapp process. The effect of phonon drag is not considered in this paper.
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Denjiro Watanabe
1959 Volume 14 Issue 4 Pages
436-443
Published: April 05, 1959
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Using a high temperature electron diffraction camera, Cu
3Pd alloys have been investigated in thin oriented, evaporated films at temperatures below and above the critical point of order-disorder. The present work has elucidated that, in alloys of α″-phase, the line-up number of anti-phase domains and the degree of order inside domains decrease with increasing temperature in the range of 20∼40°C below the critical point, and an abrupt decrease of the line-up number of domains occurs at the critical point. In the range of 100∼150°C above the critical point, short chains of one-dimensional anti-phase domains with the same period of out-of-steps as in the ordered state remain randomly in an equilibrium state. On the other hand, anti-phase domains are absent in the alloys of α′-phase below as well as above the critical point.
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Tadatosi Hibi, Tetsuhiko Tomiki
1959 Volume 14 Issue 4 Pages
444-455
Published: April 05, 1959
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The KCl single crystal which was grown from the melt, thermally quenched, and additively coloured with potassium metal were observed electronmicroscopically using replica technique. Growth of crystallites was seen both on the outer surfaces and in the interior of the crystal when it was thermally quenched or it was coloured additively. The crystallites grew more markedly in the latter case than in the former. The mechanism by which
F centres are formed were considered.
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Tadatosi Hibi, Keiji Yada
1959 Volume 14 Issue 4 Pages
455-463
Published: April 05, 1959
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The surface changes in a given part of the same KCl crystal during colouration by X-rays and in the process of bleaching by natural light have been successively observed by using two-stage replica. A slightly modified Bradley’s method was used for making two-stage replica. By this method, the surface change at the definite position of the same KCl crystal was observed successively. According to the present results, it has been clearly confirmed that crystallites grown on the KCl crystal during X-ray colouration disappear during bleaching through the process quite reverse to the crystal growth in colouration and that the behaviour of the crystal growth and its disappearance are not simple, but very peculiar. Results obtained have been briefly discussed.
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Taira Suzuki, Mikio Yamamoto
1959 Volume 14 Issue 4 Pages
463-472
Published: April 05, 1959
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A study has been made of the influence of order-disorder on the creep of a superlattice alloy Ni
3Fe. The results obtained strongly support the dislocation-climb mechanism. The activation energy for creep, independent of applied stress, slightly increases with the degree of order: 45.8 kcal/mol for disordered and 47.5±2.0 kcal/mol for ordered phases. A discontinuity occurs at the critical temperature,
i.e., 505°C in the curves of creep rate
versus the reciprocal of temperature. A remarkable acceleration of creep has been observed on the disordered alloys below
TC, which were obtained by quenching from 800°C, as compared with the rates expected from the values above
TC. A semi-quantitative theory has been proposed for such a configurational acceleration of creep in terms of order-disorder kinetics and dislocation processes in the superlattice alloy of
AB3 f.c.c. type.
In ordered alloys, the vacancy diffusion introducing the dislocation-climb is thought to be anisotropic with regard to the orientation of slip bands. This will result a significant difference in the stress dependence of creep rates in ordered phases from the one in disordered phases as observed here.
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Shigetomo Yoshida, Toshio Ikeda
1959 Volume 14 Issue 4 Pages
473-477
Published: April 05, 1959
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The absorption spectra ranging from 360 to 960 mμ were measured on rock salt crystals bombarded with electrons at various temperatures. Three types of color centers, namely
F, 590 mμ and colloidal centers were formed as a function of specimen temperature during bombardment. The thermal bleaching of these three color centers was also investigated.
From these results it is supposed that the color center with an absorption peak at about 590 mμ may correspond to a precursor of colloidal sodium. It is also suggested that there may be a correlation between coloration and dissociation of sodium chloride by electron bombardment.
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Keiji Maeda
1959 Volume 14 Issue 4 Pages
478-486
Published: April 05, 1959
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For Ca
3(PO
4)
2:Cu phosphor, measurements of spectral distributions of luminescence, reflectivity and quantum efficiency, temperature dependence of luminescence intensity and decay constants are carried out. The onedimensional configurational coordinate curves for the luminescence center in this phosphor are determined by analysing spectral data. Some characteristics expected from these curves are compared with the observed; the agreement in the absorption band width and the disagreement in the activation energy for nonradiative transition are obtained. The relations between one- and many-dimensional models are investigated and the cause for the above disagreement is attributed to the simplicity of the assumed model. Discussions are also made on the nonradiative transitions in this center.
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Masao Kuriyama
1959 Volume 14 Issue 4 Pages
487-492
Published: April 05, 1959
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Polish layer of gold was examined by means of the transmission method of electron diffraction. The diffraction pattern from the highly polished layer of gold (the Beilby layer) consists of three haloes, as reported in the previous paper (J. Phys. Soc. Japan
12 (1957) 151). The radial distribution function of atoms in the layer was calculated by Fourier transformation of the observed intensity. The observed intensity was compared with those calculated from appropriate models of atomic arrangement. It was found that the Beilby layer has an amorphous arrangement in which the first and the second coordination number are about 10 and 8, respectively.
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Junkichi Itoh, Riichiro Kusaka
1959 Volume 14 Issue 4 Pages
492-498
Published: April 05, 1959
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Nuclear magnetic double resonance studies were done on two proton system in K
2HgCl
4·H
2O single crystal. Applying a strong r.f. field with the frequency nearly equal to that of one line in the doublet of two proton resonance, the line shape of the other line of the doublet was measured for various values of the intensity and frequency of the strong r.f. field. Generally, the observed line shape shows further doublet structure, and the separation and relative intensities of this doublet depend upon the intensity and frequency of the strong r.f. field. Some calculations were made for the line structure of two proton system under the influence of a strong r.f. field. The experimental results agree qualitatively with the calculation, but there exist some descrepancies in the absolute magnitudes of the splitting of the induced doublet.
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Masatoshi Yamazaki
1959 Volume 14 Issue 4 Pages
498-510
Published: April 05, 1959
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The electronic structure of the ground state of the protonated methane
CH+5 is studied by the Heitler-London-Slater-Pauling method extended by Voge and by Kotani and Siga. The wave functions are constructed without the assumption of the electron pair bond and with taking (2
s)
2(2
p)
2, (2
s)(2
p)
3, and (2
p)
4 configurations of the carbon atom into account. Assuming a probable model for this ion, we obtain seventeen
1A1′ states. The energy matrix for these states is computed by means of the representation matrices of the symmetric group. By solving the secular equations thus obtained for two different sets of parameters, the binding energy (or the proton affinity) and the equilibrium proton-carbon distance are estimated.
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Hiroshi Watanabe
1959 Volume 14 Issue 4 Pages
511-516
Published: April 05, 1959
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LaFeO
3, which is reported to be antiferromagnetic at room temperature, has, however, a small amount of remanent magnetization. By measuring the hysteresis loops of a sample before and after a thermomagnetic treatment, it is found that the hysteresis loop is shifted along the magnetization axis, especially for specimens cooled in a magnetic field below the magnetic transition temperature,
ca 450°C. The phenomenon can well be interpreted as a sort of thermo-remanent magnetization. A similar phenomenon has also been found for NdFeO
3.
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Hideo Takami
1959 Volume 14 Issue 4 Pages
517-522
Published: April 05, 1959
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Stability of two-dimensional Szymanski flow
Stability of a two-dimensional transient flow of an incompressible viscous fluid is investigated by the method of small oscillations. The basic flow is such that the fluid begins to move from rest between two parallel and infinitely large planes under a pressure of constant gradient applied along them and eventually attains the parabolic velocity distribution.
By the use of Lin’s procedure the relation between the Reynolds number of the basic flow and the wave number of the antisymmetrical neutral oscillation (the neutral curve of stability) and also the minimum critical Reynolds number are calculated numerically for each of five representative stages of the transient flow, and the variation of its stability characteristics is discussed.
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Sinzi Kuwabara
1959 Volume 14 Issue 4 Pages
522-527
Published: April 05, 1959
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Using Imai’s general method of solving two-dimensional Oseen’s equations, the drag and lift coefficients for a lattice of parallel, equal and equidistant elliptic cylinders in a uniform flow at small Reynolds numbers are calculated. When the stagger is not present and the thickness ratio of the elliptic cylinders is taken to be unity, the expressions for these coefficients reduce to the case of a lattice of equal and equidistant circular cylinders which has been investigated by Tamada and Fujikawa.
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Sinzi Kuwabara
1959 Volume 14 Issue 4 Pages
527-532
Published: April 05, 1959
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The forces experienced by parallel circular cylinders or spheres which are distributed at random and homogeneously in a viscous flow are investigated on the basis of Stokes’ approximation. The results for the case of spheres are applied to the problem of sedimentation and compared with several experimental data.
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Shigeyoshi Kittaka
1959 Volume 14 Issue 4 Pages
532-538
Published: April 05, 1959
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The generation of static electricity by the contact and seperation between high polymer substances and metals has been studied. The couples of polystyrene-Pt, Acrylite (polymethylmethacrylate)-Pt, and Teflon (polytetrafluoroethylene)-Pt were examined. It was observed that the surrounding conditions have serious effects on the quantity and sign of generated static charge.
The mechanism of generation of electro-static charge has been proposed assuming the energy levels of the localized electrons on the surface of high polymer substances and the change of these energy levels by the absorption of different gases. It was estimated that work functions of polystyrene, Acrylite, and Teflon are 5.74 eV, 5.48 eV and 6.04 eV, respectively.
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Sadaaki Yanagawa
1959 Volume 14 Issue 4 Pages
539
Published: April 05, 1959
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Surjit Singh
1959 Volume 14 Issue 4 Pages
540
Published: April 05, 1959
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Seiichi Tanuma
1959 Volume 14 Issue 4 Pages
541
Published: April 05, 1959
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Setsuo Okanishi, Hitoshi Kanamori
1959 Volume 14 Issue 4 Pages
542
Published: April 05, 1959
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Kuniya Fukuda, Hiroaki Matumoto, Yoichi Uchida, Hisamitsu Yoshimura
1959 Volume 14 Issue 4 Pages
543
Published: April 05, 1959
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Shintaro Sugai, Mitsuo Ishikawa, Jiro Furuichi
1959 Volume 14 Issue 4 Pages
544
Published: April 05, 1959
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Tosio Kato, Hiroshi Fujita
1959 Volume 14 Issue 4 Pages
545
Published: April 05, 1959
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Masayasu Ueta, Masamitsu Hirai
1959 Volume 14 Issue 4 Pages
546
Published: April 05, 1959
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Keiichi Ando, Osami Kamigaito, Yoshihiro Kamiya, Shigetoshi Takahashi, ...
1959 Volume 14 Issue 4 Pages
547A
Published: April 05, 1959
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Nisiki Hayasi
1959 Volume 14 Issue 4 Pages
547B
Published: April 05, 1959
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Kazuyuki Ogawa
1959 Volume 14 Issue 4 Pages
547C
Published: April 05, 1959
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