Journal of the Physical Society of Japan

Magnetic Moment of F¹⁷ —Nuclear Magnetic Resonance by Polarization Following O¹⁶ (d, n) F¹⁷ Reaction—

Kenzo Sugimoto, Akira Mizobuchi, Kozi Nakai, Kozi Matuda

1966 Volume 21 Issue 2 Pages 213-221
Published: February 05, 1966
Released on J-STAGE: June 01, 2007

DOIhttps://doi.org/10.1143/JPSJ.21.213

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The nuclear magnetic resonance of F¹⁷ (T_1⁄2=66 sec) has been observed using the polarization of recoil nuclei produced by the reaction O¹⁶ (d, n) F¹⁷ and the β-decay anisotropy as the indicator of the polarization. The accomplishment of the experiment was essentially due to the persistence of the polarization by specific experimental methods, i.e., the use of a strong magnetic field (\gtrsim5 kG) in the direction of polarization and the use of pure CaF₂ crystals as the stopping material of recoil ions. The observed asymmetry of β-counting was about 2% and a spin relaxation time T₁ comparable to the half-life of F¹⁷ was observed. The value obtained of the magnetic moment of F¹⁷ is μ=4.7224±0.0012 nm with the diamagnetic correction.

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The Magnetic Anisotropy Induced by Electron Diffusion in Co_1+2xFe_2−2xO₄ and Fe_1−2xNi_2xCo₂O₄

Tetsutaro Iizuka, Shuichi Iida

1966 Volume 21 Issue 2 Pages 222-231
Published: February 05, 1966
Released on J-STAGE: May 29, 2007

DOIhttps://doi.org/10.1143/JPSJ.21.222

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A detailed study of the magnetic anisotropy of a Co_1.1Fe_1.9O₄ single crystal at 77°K revealed that, after cooling in a magnetic field, a relatively small uniaxial anisotropy is superposed on the large cubic anisotropy (K₁ and K₂). Rotational hysteresis is present at 77°K which is explained in terms of the irreversible wall displacement and the relaxing anisotropy energy. The presence of large rotational hysteresis in polycrystalline specimens CoFe₂O₄∼Co₃O₄ is also shown and is explained on this basis. Preliminary data on the relaxation time of the phenomenon are presented. All the data are consistent with the mechanism presented by Mizushima, which assumes the electron diffusion between Co²⁺ and Co³⁺ions. Data in the series Fe_1−2xNi_2xCo₂O₄ are also presented. Suggestions are made that the rotational hystereses observed in Co₂Ba₂Fe₁₂O₂₂ and BaCo_δTi_δFe_12−2δO₁₈ at low temperatures are caused by the same mechanism.

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Dynamic Properties of Permalloy Thin Films

Gen Matsumoto, Takeo Satoh, Shuichi Iida

1966 Volume 21 Issue 2 Pages 231-237
Published: February 05, 1966
Released on J-STAGE: June 01, 2007

DOIhttps://doi.org/10.1143/JPSJ.21.231

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Free oscillations, switching and ferromagnetic resonance of Permalloy thin films are measured changing, for each film, various parameters including temperature. It is shown that the damping factor λ in the free oscillations of Permalloy thin film is composed of three parts as
λ=λ_in+λ_edd+kH_y,
where λ_in is due to the intrinsic damping plus the damping from the anisotropy dispersion, λ_edd due to the eddy current damping, which is represeted as 1.0×10¹⁷d² (cps) as a function of the thickness d, and kH_y due to the high power effect probably caused by the increased excitation of the spin wave modes. In the last term H_y is the amplitude of the applied pulse field and k is a constant which depends on the film thickness. The value of λ_in is about 1.05×10⁸ (cps) and is in good agreement with the minimum value of λ ever obtained for Permalloy films by various measurements.

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Magnetocrystalline Anisotropy and Magnetostriction of the Intermetallic Compound Fe₅Ge₃

Yoshio Tawara

1966 Volume 21 Issue 2 Pages 237-243
Published: February 05, 1966
Released on J-STAGE: June 01, 2007

DOIhttps://doi.org/10.1143/JPSJ.21.237

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Magnetocrystalline anisotropy constants of Fe₅Ge₃ were determined as K₁=−5.1×10⁶erg/cm³, |K₃|=1.2×10²erg/cm³ for room temperature and K₁=−8.4×10⁶erg/cm³, |K₃|=1.6×10²erg/cm³ for liquid nitrogen temperature by means of torque measurements. The temperature dependence of K₁ can be well interpreted by a one ion anisotropy model based on the Kanematsu’s spin scheme and the molecular field approximation. Magnetostriction of the crystal at room temperature was studied by using strain gauges. Magnetostriction constants were determined as λ(001,100)=−20×10⁻⁶, λ(001,001)=32×10⁻⁶ and λ(010,100)=6.7×10⁻⁶. These values are qualitatively consistent with the one ion anisotropy model.

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Quantum Oscillation of Electromagnetic Wave Absorption in Metals

Shoichi Mase

1966 Volume 21 Issue 2 Pages 243-254
Published: February 05, 1966
Released on J-STAGE: June 01, 2007

DOIhttps://doi.org/10.1143/JPSJ.21.243

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The observability of the quantum oscillation (Shubnikov-de Haas oscillation) in optical absorption and microwave absorption in metals or semimetals in the normal skin effect region is investigated for typical cases of relative directions of magnetic field and wave propagation. The unobservably small or observable but small quantum oscillation in most existing experimental results is reasonably understood from this study, while the existence of greatly enhanced quantum oscillation in both longitudinal and transverse magnetoreflections at the plasma reflection edge is predicted. Further it is also predicted that this purely quantum oscillation at the plasma edge should appear in Faraday rotation and Voigt phase shift with great amplitude.

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Nuclear Magnetic Resonance Studies of Beryllium-Based Laves Phase XBe₂

Haruo Saji, Tokio Yamadaya, Mitsuru Asanuma

1966 Volume 21 Issue 2 Pages 255-261
Published: February 05, 1966
Released on J-STAGE: June 01, 2007

DOIhttps://doi.org/10.1143/JPSJ.21.255

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The nuclear magnetic resonance (NMR) of Be⁹ has been investigated with several beryllium-Laves phase intermetallic compounds TiBe₂, CrBe₂, MnBe₂ and CuBe₂ at various temperatures from 77°K to 300°K. The Knight shift of Be⁹ resonance was found to be constant: (∼−0.01%) in CrBe₂ and (∼−0.06%) in MnBe₂ at all temperatures. In TiBe₂ the shift of Be⁹ resonance depends on temperature, and varies from (−0.08%) to (−0.04%) in the temperature range from 77°K to 300°K.
The NMR of Mn⁵⁵ in MnBe₂ and Ti⁴⁷+Ti⁴⁹ in TiBe₂ have also been observed. The shift of Mn⁵⁵ resonance was (∼−0.8%), which was temperature independent, while that of Ti⁴⁷+Ti⁴⁹ varied from (∼−0.5%) to (∼+0.07%) in the temperature range from 77°K to 300°K.
As for Ti⁴⁷+Ti⁴⁹ resonance, the relation between the Knight shift (K) and the susceptibility (χ) is linear. From the K vs. χ curve the apparent hyperfine field can be estimated at 27Koe/spin. This small value of hyperfine field may be considered to have resulted from a mixture of s character into the d wave functions. A simple band mode is proposed to account for the NMR properties of these compounds.

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Jahn-Teller Effects on Mössbauer Spectra of Fe₅₇ in FeCr₂O₄ and FeV₂O₄

Midori Tanaka, Tetsuzi Tokoro, Yoshimichi Aiyama

1966 Volume 21 Issue 2 Pages 262-267
Published: February 05, 1966
Released on J-STAGE: May 29, 2007

DOIhttps://doi.org/10.1143/JPSJ.21.262

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Mössbauer spectra of FeCr₂O₄ and FeV₂O₄, which undergo the cubic-to-tetragonal transition at 135°K and 140°K respectively, have been measured in the temperature range from liquid nitrogen to room temperature. Quadropole splittings have been observed even above the distortion temperature. Each line of the Mössbauer spectra becomes broadest at the transition temperature. These temperature dependence of the Mössbauer spectra can be explained qualitatively on the basis of the simple model of a motional narrowing phenomenon.

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Electron Spin Resonances in Reduced BaTiO₃

Takeshi Takeda, Akinori Watanabe

1966 Volume 21 Issue 2 Pages 267-274
Published: February 05, 1966
Released on J-STAGE: May 29, 2007

DOIhttps://doi.org/10.1143/JPSJ.21.267

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Electron spin resonances of reduced BaTiO₃ were observed in X band at 77°K and 55°K. The paramagnetic centers in the crystals reduced at temperatures between 650°C and 1000°C have three equivalent sites, each of which shows tetragonal symmetry. The g tensor is axial symmetric: g_⁄⁄=1,930 and g_⊥=1,911. Spin-lattice relaxation time is of the order of 10⁻⁶ s at 55°K. Resonance of impurity Pt³⁺ disappears in the crystals reduced at above 650°C. These facts indicate that the center observed is an F-center surrounded by two Ti⁴⁺ and four Ba²⁺ ions. Another kind of complex centers appear in the crystals reduced at 1100°C. The origin of these centers, however, has not been analyzed yet. With the crystals reduced at 1300°C, the two kinds of centers mentioned above completely vanish. This is due to purge of electron traps.

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Antiferromagnetism of Disilicides of Heavy Rare Earth Metals

Kazuko Sekizawa, Ko Yasukochi

1966 Volume 21 Issue 2 Pages 274-278
Published: February 05, 1966
Released on J-STAGE: May 29, 2007

DOIhttps://doi.org/10.1143/JPSJ.21.274

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Magnetic properties of disilicides of Gd, Tb, Dy, Ho, and Er have been investigated at temperatures ranging from 4.2°K to room temperature. All the disilicides except ErSi₂ have the orthorhombic ThSi₂ type of crystal structure and are shown to be antiferromagnetic. The Néel temperatures of GdSi₂, TbSi₂, DySi₂, and HoSi₂ are 27°K, 17°K, 17°K, and 18°K, respectively. The compound ErSi₂ has the hexagonal AlB₂ type of crystal structure and is paramagnetic at above 4.2°K. The paramagnetic Curie temperature of these compounds decreases with the number of f electrons of the rare earth ion.

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Magnetic Susceptibility and Electronic Specific Heat of Transition Metals and Alloys. VIII. Hf, Ta, W and Re Metals and Their Alloys

Atsushi Katsuki, Masao Shimizu

1966 Volume 21 Issue 2 Pages 279-286
Published: February 05, 1966
Released on J-STAGE: June 01, 2007

DOIhttps://doi.org/10.1143/JPSJ.21.279

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The temperature variations of electronic specific heats and spin paramagnetic susceptibilities without molecular field are calculated for Hf, Ta, W and Re metals and their alloys by making use of the density of states determined from low temperature specific heat data for 5d-group transition metals and their alloys. Calculated results qualitatively explain the temperature variations of the estimated electronic specific heats for these metals. By comparing the calculated results of spin paramagnetic susceptibilities with the experimental data on magnetic susceptibilities, the values of molecular field coefficient, α, and additional constant paramagnetic susceptibility, χ_c, are estimated for these metals and alloys, and the composition dependence of χ_c is shown. A brief discussion on the NMR shift for Ta and W metals is given.

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Anisotropic s-f Interaction in Rare Earth Metals. I. Fundamental Consideration Based on the Free Electron Model

T. Kasuya, D. H. Lyons

1966 Volume 21 Issue 2 Pages 287-307
Published: February 05, 1966
Released on J-STAGE: June 01, 2007

DOIhttps://doi.org/10.1143/JPSJ.21.287

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General treatment of the s-f anisotropic exchange interaction is given based on the formulation of Kaplan and Lyons. The free electron model is assumed, and the results given as an expansion in k_f\barr_f. Various types of induced f-f interactions are also obtained as an expansion in k_f\barr_f. The range of these f-f interactions is shown to increase with the order. The contribution to the electrical resistivity is also given together with the contribution from screened multipole scattering. Qualitative comparison with actual rare earth metals may be made by using a more realistic band model.

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Electronic Properties for Pd Metal and Its Ferromagnetic Alloys —On the Number of Holes in the 4d-Band of Pd Metal—

Hatsuo Kimura, Atsushi Katsuki, Masao Shimizu

1966 Volume 21 Issue 2 Pages 307-312
Published: February 05, 1966
Released on J-STAGE: June 01, 2007

DOIhttps://doi.org/10.1143/JPSJ.21.307

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By making use of a new experimental fact that the number of electrons in the 5s-band or the number of holes in the 4d-band is 0.36 per atom for Pd metal, the composition dependence of the magnetization of Pd–Fe and Pd–Co alloys is discussed, and residual electric resistivities for Ni–Pd alloys are calculated. Using the density of states curve which has been determined. from the low temperature specific heat data and modified by taking account of this new fact, the temperature dependence of the electronic specific heat and the paramagnetic susceptibility of Pd metal is calculated. The new value of the number of holes or electrons can give better interpretation of the experimental results than the value 0.6 per atom, which has so far been believed to be most probable.

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Magnetic Domain Pattern and Magnetocrystalline Anisotropy in Epitaxially Grown Thin Films of Fe, Ni, and Ni–Fe Alloys

Sonoko Tsukahara, Hisazo Kawakatsu

1966 Volume 21 Issue 2 Pages 313-325
Published: February 05, 1966
Released on J-STAGE: May 29, 2007

DOIhttps://doi.org/10.1143/JPSJ.21.313

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Crystal grains and domain patterns of Ni–Fe alloy films which were condensed on cleaved surfaces of heated NaCl in a vacuum of 5×10⁻⁵ torr were studied by transmission electron microscopy and electron diffraction. Magnetic anisotropy was also measured by a torque magnetometer for thin films. The substrate temperature was varied between room temperature and 600°C. The films obtained range from polycrystal to nearly perfect single crystals. The degree of perfection of the crystal is classified into several types. The magnetic domain patterns and crystal anisotropies of the films depend on the composition and also on the degree of perfection of the films. Polycrystalline films are, in general, found to consist of domains of irregular shapes with curved walls and ripple structure within the domains. In good epitaxial films, however, the domains have a regular cross-hatched shape and when the films are magnetized parallel to one of the crystal anisotropy axes, the films are composed of linear domain walls almost without any ripple. Ni films, which have a large magnetostriction are apt to be influenced by internal and external stresses, which affect the domain pattern and the torque curve. Even for good epitaxial Ni films the stress induced anisotropy is often superior to the crystal anisotropy.
The measured values of crystal anisotropy constant K₁ of good epitaxially grown films of Ni–Fe alloys agree with those of the bulk materials, but, in pure Ni and pure Fe films, they are 1.5–2 times as large as the bulk values.

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Dynamical Theory of Diffraction. I. Electron Diffraction

Y. H. Ohtsuki, S. Yanagawa

1966 Volume 21 Issue 2 Pages 326-335
Published: February 05, 1966
Released on J-STAGE: June 01, 2007

DOIhttps://doi.org/10.1143/JPSJ.21.326

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A quantum field theoretical method is applied to the dynamical theory of electron diffraction. It is shown by making use of a Green function which has been developed in the field of many body problems that the dispersion equation and the absorption coefficient of the dynamical theory can be obtained from the calculation of the pole of the Green function. The effective Hamiltonian which is used for the calculation of the Green function is derived by a diagram method of the Green function. The amplitude ratios of diffracted waves are given by the ratios of Fourier components of the Green function.

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Crystallization of Amorphous Titanium Dioxide Films Prepared by Vacuum-Evaporation

Makoto Shiojiri

1966 Volume 21 Issue 2 Pages 335-345
Published: February 05, 1966
Released on J-STAGE: May 29, 2007

DOIhttps://doi.org/10.1143/JPSJ.21.335

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An electron microscopy and electron diffraction study was made on the structure of vacuum-deposited films of titanium dioxide. The films were amorphous when they were deposited on rocksalt at room temperature. When irradiated by an intense electron beam, the amorphous films crystallized in anatase and rutile forms. The rutile crystallities were small granules, whereas the anatase crystals grew to occupy larger areas of several microns in linear dimension. The difference in structure of the crystallized films seemed to be originated in the intrinsic properties of the amorphous films. The generation of dislocations which constituted small angle grain boundaries was observed in growing anatase crystals. In these crystals, twins were formed on the {112} planes and dislocations were also observed in the individual grains.

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Epitaxial Growth of Metals on Rocksalt Faces Cleaved in Vacuum. II. Orientation and Structure of Gold Particles Formed in Ultrahigh Vacuum

Shozo Ino

1966 Volume 21 Issue 2 Pages 346-362
Published: February 05, 1966
Released on J-STAGE: May 29, 2007

DOIhttps://doi.org/10.1143/JPSJ.21.346

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The orientation and structure of gold particles formed by evaporation on rocksalt cleaved in ultrahigh vacuum have been studied at various stages of the nucleation and growth process. Besides four 200 and twenty-four 220 spots which indicate the presence of the (001) orientation and (111) orientation respectively, twenty-four abnormal 111 spots have been observed in electron diffraction patterns taken at earlier stages of growth, and various unusual contrasts have been observed in dark field electron micrographs using one of 111 spots. A multiply twinned particle model is proposed by the present author, and the appearance of the 111 spots and the dark field image contrasts can satisfactorily be explained by this model. With increasing thickness particles with the (111) orientation and without the multiple twinning exclusively grow up, while multiply twinned particles and those with the (001) orientation seem to stop their growth; and a continuous gold film with the (111) fibrous structure is formed at a thickness of about 500 Å.

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Nature of Slow Electron Diffraction by Crystals

Shizuo Miyake, Kazunobu Hayakawa

1966 Volume 21 Issue 2 Pages 363-378
Published: February 05, 1966
Released on J-STAGE: June 01, 2007

DOIhttps://doi.org/10.1143/JPSJ.21.363

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By making use of a new slow-electron diffraction apparatus of display type which is provided with the freedom of changing the glancing and azimuthal angles of the crystal and enables the pattern observation over a wide range of scattering angle by using cylindrical accelerating grids and fluorescent screen, the general feature of diffraction patterns from the cleavage surface of zincblende is studied with electrons in the energy range from 90 V to 500 V.
A number of diffraction effects which are to be ascribed to the interactions among simultaneously excited reflexions are revealed. Since it would undoubtedly be necessary to use the dynamical theory of diffraction for explaining them, the way of approach to the slow electron diffraction phenomena with this theory and also the speciality of this theory for slow electrons are discussed from a general point of view, referring to observation of the high-energy electron diffraction from the same crystal surface. In particular, the conception of the penetration depth and the absorption effect of slow electrons in the crystal are critically discussed.

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A Method of Realizing the Minimum-B Field

Taro Sometani, Kenzo Yamamoto

1966 Volume 21 Issue 2 Pages 379-384
Published: February 05, 1966
Released on J-STAGE: June 01, 2007

DOIhttps://doi.org/10.1143/JPSJ.21.379

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The minimum-B field is calculated in series or characteristic functions of Laplace’s equation. It is shown that a magnetic field can be realized if the current is so distributed that the terms of higher orders in the field components are cancelled out while those of lower orders are reserved. Such current distribution can be approximately realized by using suitable a combination of current carrying conductors.

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Non-Linear Hydromagnetic Waves Propagating along a Magnetic Field in a Cold Collision-Free Plasma

Tsunehiko Kakutani

1966 Volume 21 Issue 2 Pages 385-391
Published: February 05, 1966
Released on J-STAGE: June 01, 2007

DOIhttps://doi.org/10.1143/JPSJ.21.385

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Non-linear hydromagnetic waves propagating along a uniform magnetic field in a cold collision-free plasma are dealt with. It is assumed that the plasma is fully ionized and quasi-neutral, and that the loop-motion of the plasma particles does not occur.
The solutions of the problem are divided into two classes according as l is equal to zero or not, where l is a parameter relating to the angular momentum flux carried by the plasma particles in the direction of the uniform magnetic field. In both cases, exact solutions representing wave-trains can be obtained in terms of Jacobian elliptic functions. In particular, the first class (l=0) includes an isolated pulse solution as a special case.

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A New Emission Band in Cubic Cadmium Sulfide

Seizo Toyotomi, Yoshikazu Sugiura

1966 Volume 21 Issue 2 Pages 392
Published: February 05, 1966
Released on J-STAGE: May 29, 2007

DOIhttps://doi.org/10.1143/JPSJ.21.392

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Mn⁵⁵ Nuclear Magnetic Resonance of Mn²⁺ Ions Located at B-Sites in Manganese Ferrite

Hiroshi Yasuoka

1966 Volume 21 Issue 2 Pages 393
Published: February 05, 1966
Released on J-STAGE: June 01, 2007

DOIhttps://doi.org/10.1143/JPSJ.21.393

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Uniaxial Stress Effects on Electrical Conductivity of DPPH Single Crystal

Mitsuo Kawabe, Kohzoh Masuda, Jiro Yamaguchi, Yoshinobu Aoyagi

1966 Volume 21 Issue 2 Pages 394
Published: February 05, 1966
Released on J-STAGE: May 29, 2007

DOIhttps://doi.org/10.1143/JPSJ.21.394

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Absorption Edges of NaCl Single Crystal

Takeo Miyata, Tetsuhiko Tomiki

1966 Volume 21 Issue 2 Pages 395
Published: February 05, 1966
Released on J-STAGE: June 01, 2007

DOIhttps://doi.org/10.1143/JPSJ.21.395

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Effects of Atmospheres on the Formation of Secondary Defects in Quenched Pure Aluminum

Yoshiharu Shimomura, Yoshinori Manmoto, Sho Yoshida

1966 Volume 21 Issue 2 Pages 396
Published: February 05, 1966
Released on J-STAGE: May 29, 2007

DOIhttps://doi.org/10.1143/JPSJ.21.396

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Electron Spin Resonance of (KMnF₃)_x(KMgF₃)_1−x

Kazumi Horai, Kunio Saiki

1966 Volume 21 Issue 2 Pages 397
Published: February 05, 1966
Released on J-STAGE: June 01, 2007

DOIhttps://doi.org/10.1143/JPSJ.21.397

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V Bands in KCl:I Crystal

Sadao Hattori, Nobuyoshi Nagata

1966 Volume 21 Issue 2 Pages 398
Published: February 05, 1966
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DOIhttps://doi.org/10.1143/JPSJ.21.398

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Perpendicular Anisotropy in Nickel-Iron Magnetic Thin Films Evaporated at Low Substrate Temperatures

Tosiaki Koikeda, Soshin Chikazumi

1966 Volume 21 Issue 2 Pages 399
Published: February 05, 1966
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DOIhttps://doi.org/10.1143/JPSJ.21.399

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Shifts of Electron Diffraction Spots of Cu–Al Martensite Transformed in Thin Foils

Setsuo Kajiwara, Hiroshi Fujita

1966 Volume 21 Issue 2 Pages 400
Published: February 05, 1966
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DOIhttps://doi.org/10.1143/JPSJ.21.400

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Effective In-Plane Anisotropy and Trigonal Magnetostriction in α-Fe₂O₃

Shuichi Iida, Koichi Mizushima

1966 Volume 21 Issue 2 Pages 401-402
Published: February 05, 1966
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DOIhttps://doi.org/10.1143/JPSJ.21.401

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Effect of a Transverse dc Biasing Field on the Longitudinal M-H Loops along an Easy Axis for Biaxial Magnetic Thin Films

Yasushi Kamo, Shu Chiba

1966 Volume 21 Issue 2 Pages 402
Published: February 05, 1966
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DOIhttps://doi.org/10.1143/JPSJ.21.402

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Absorption Edges of KCl Single Crystals

Tetsuhiko Tomiki

1966 Volume 21 Issue 2 Pages 403-404
Published: February 05, 1966
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DOIhttps://doi.org/10.1143/JPSJ.21.403

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Magnetocrystalline Anisotropy of Fe₂B

Atsushi Iga, Yoshio Tawara, Akira Yanase

1966 Volume 21 Issue 2 Pages 404
Published: February 05, 1966
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DOIhttps://doi.org/10.1143/JPSJ.21.404

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Magnetic Properties of GdSi₂

Koichi Yaguchi

1966 Volume 21 Issue 2 Pages 405A
Published: February 05, 1966
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DOIhttps://doi.org/10.1143/JPSJ.21.405A

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Atomic Parameters in Ferroelectric SbSI

Yoshio Oka, Atsushi Kikuchi, Toshio Mori, Etsuro Sawaguchi

1966 Volume 21 Issue 2 Pages 405B-406B
Published: February 05, 1966
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DOIhttps://doi.org/10.1143/JPSJ.21.405B

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Alloy Hardening of Cu–Si Solid Solution at 4.2°K

Koji Kamada

1966 Volume 21 Issue 2 Pages 406-407
Published: February 05, 1966
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DOIhttps://doi.org/10.1143/JPSJ.21.406

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A Study on Spin Structure of Mn(HCOO)₂·2H₂O

Kazuo Yamagata, Hidetaro Abe

1966 Volume 21 Issue 2 Pages 408-409
Published: February 05, 1966
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DOIhttps://doi.org/10.1143/JPSJ.21.408

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UV Reflection Spectra of KCl Single Crystals

Tetsuhiko Tomiki

1966 Volume 21 Issue 2 Pages 409-410
Published: February 05, 1966
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DOIhttps://doi.org/10.1143/JPSJ.21.409

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Transport Phenomena in Indium Antimonide at Higher Electric Field

Hiroshi Morisaki, Yoshio Inuishi

1966 Volume 21 Issue 2 Pages 411A
Published: February 05, 1966
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DOIhttps://doi.org/10.1143/JPSJ.21.411A

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Current Saturation Associated with Ultrasonic Amplification in CdS Crystals

Akira Ishida, Chihiro Hamaguchi, Yoshio Inuishi

1966 Volume 21 Issue 2 Pages 411B
Published: February 05, 1966
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DOIhttps://doi.org/10.1143/JPSJ.21.411B

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High Power Behavior and Spin-wave Spectrum in a Hexagonal Ferrite with Large Planar Anisotropy

Masaru Mita

1966 Volume 21 Issue 2 Pages 411C
Published: February 05, 1966
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DOIhttps://doi.org/10.1143/JPSJ.21.411C

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Optical Absorption in Noble Metals

Eijiro Haga, Hiroaki Okamoto

1966 Volume 21 Issue 2 Pages 411D
Published: February 05, 1966
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DOIhttps://doi.org/10.1143/JPSJ.21.411D

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Field-Induced Transitions in the Hematite Crystal

Takejiro Kaneko, Shunya Abe

1966 Volume 21 Issue 2 Pages 412A
Published: February 05, 1966
Released on J-STAGE: May 29, 2007

DOIhttps://doi.org/10.1143/JPSJ.21.412A

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Band Structure of Metallic Copper and Nickel by a Self-Consistent Procedure

Shinya Wakoh

1966 Volume 21 Issue 2 Pages 412B
Published: February 05, 1966
Released on J-STAGE: May 29, 2007

DOIhttps://doi.org/10.1143/JPSJ.21.412B

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Crystal Structure and Magnetic Property of FeMnAs

Shizuka Yoshii, Hisao Katsuraki

1966 Volume 21 Issue 2 Pages 412C
Published: February 05, 1966
Released on J-STAGE: May 29, 2007

DOIhttps://doi.org/10.1143/JPSJ.21.412C

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