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Y. P. Varshni
1974 Volume 36 Issue 2 Pages
317-325
Published: February 15, 1974
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A detailed analysis of the applicability of two three-parameter expressions for the level energies has been carried out on the ground-state bands of 149 deformed even-even nuclei. It is shown that the expression
EI=
aI(
I+1)+
pI+
qI2(
I+1), provides a satisfactory description of the experimental data and gives better results amongst the two. A method of estimating
Ic, the spin at which the “back-bending” effect is expected to take place, is also developed.
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S. S. Bhati, Nirmal Singh, P. C. Mangal, P. N. Trehan
1974 Volume 36 Issue 2 Pages
326-330
Published: February 15, 1974
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Angular correlation studies have been carried out for seven cascades viz. 275–410, 275–319, 596–91, 440–91, 398–91, 319–91 and 197–398 keV in
147Pm. Out of these 275–410 keV cascade has been attempted for the first time. A spin assignment of 5/2
+ has been confirmed for the 490 keV level. The mixing ratios of 596, 440, 410, 398, 319 and 197 keV gamma rays were found to be M1+(19
−4+6)% E2, M1+(25
−3+4)% E2, E2+3.8% M3, M1+(5±1.5)% E2, M1+(1.5
−1.5+1.0)% E2 and M1+(82±4)% E2, respectively. The experimental transition probabilities for the 596, 440, 275, 197 and 91 keV gamma rays have been calculated and comparison made with the single particle estimates.
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Shoji Shirato, Kazuo Saitoh
1974 Volume 36 Issue 2 Pages
331-335
Published: February 15, 1974
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The revised data of the n-p differential cross section at 14.1 MeV have been presented. The revised values of the cross section at 8 mean neutron-scattering angles in the range 172.0°–52.5° in the C. M. system have been increased systematically by about 2.3% than our previous values due to the precisely calculated neutron-flax correction. The result of a re-measurement done by using a new polyethylene radiator and a new neutron-source apparatus is in good agreement with the revised data.
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Eiko Takekoshi, Yoshihide Ishizaki, Hikonojo Orihara, Masaaki Kanazawa ...
1974 Volume 36 Issue 2 Pages
336-340
Published: February 15, 1974
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The (p, t) reaction at
Ep=52 MeV has been used to study differential cross sections and cross section ratios of the ground state band members in
236U and
230Th. Experimental results were compared with the usual zero-range DWBA calculations, where the difference between deformations of the target and the residual nucleus was explicitly taken into account. In
236U angular distributions of 0
+(g. s), 2
+(45 keV), 4
+(149 keV) and 6
+(310 keV) members of ground state band were obtained. In addition, the 8
+(520 keV) member, which has been assigned from α-γ measurements, was observed. For
230Th, the 0
+(g. s), 2
+(53 keV) and 4
+(174 keV) members of the ground-state band were observed and also the previously unobserved 6
+ member was found at an excitation energy very near that 400 keV estimated from the I(I+1) law.
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Yoji Totsuka, Masatoshi Koshiba
1974 Volume 36 Issue 2 Pages
341-350
Published: February 15, 1974
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A method of phenomenological analysis of multiple muon events is presented, where the influence of the decay probability of parent mesons are explicitly taken into account and the effect of the finite size of detectors are also included. Our experimental results as well as other existing data deep underground were analysed and mutually consistent reasonable fits were obtained for the existing data.
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Teruhiro Suda, Yoji Totsuka, Masatoshi Koshiba
1974 Volume 36 Issue 2 Pages
351-360
Published: February 15, 1974
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An experiment was carried out at vertical depths of 1350 hg/cm
2 underground in order to investigate the high energy, \gtrsim450 GeV, muon bundles. The muon bundles, upto the highest observed multiplicity of 18, were observed in a stack of three horizontal layers of wide gap spark chambers and three lead absorber layers of area 8.35 m
2 each.
The experimental set-ups and the procedures in correcting for various experimental biases are described. The result for the average zenith angle of 20° and the average slant depth of 1380 hg/cm
2 in standard rock is presented in the from of multiplicity distribution.
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Hiroshi Yasuhara
1974 Volume 36 Issue 2 Pages
361-369
Published: February 15, 1974
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Short-range correlations in an electron gas are investigated from a diagrammatic analysis of perturbation theory. An infinite sum of electron-electron ladder diagrams is shown to be indispensable for the short-range correlation at metallic densities. A new approximate expression for the dielectric function ε(
q, ω) is presented, which is an interpolation between the random phase approximation (RPA) for small
q and an infinite sum of ladder diagrams between electrons with antiparallel spins for large
q.
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Yoshihiro Ohmura, Koji Ishikawa, Yukio Mizuno
1974 Volume 36 Issue 2 Pages
370-375
Published: February 15, 1974
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Rigorous calculation of the same type as a preceding paper of this series is carried out for absorption spectra, and the following conclusions are drawn.
(i) Absorption spectra also follow the generalized power law like emission spectra did:
\ ilde
w(ω)=γ(ω)|ω
F−ω|
α(ω) for ω>ω
F,
where ω denotes the frequency of absorbed photon, ω
F being the value at threshold.
(ii) Both α(ω) and γ(ω) are regular at ω=ω
F, and they are exactly the analytical continuations of those for the corresponding emission spectra into the frequency range ω>ω
F, respectively.
Both (i) and (ii) are expected to remain valid as they stand or with slight extentions even for models and situations much more general and much more realistic than examined actually in papers of this series, and they will form the basis for analysing experiments.
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Yukio Osaka
1974 Volume 36 Issue 2 Pages
376-385
Published: February 15, 1974
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Hohenberg and Kohn have dealt with the ground state of an interacting electron gas in an external potential and show that there exists a universal functional of the electron density
n(
r),
G[
n(
r)], independent of an external potential. This functional plays a central role in a theory of inhomogeneous electron gas. In this paper, a formal theory for deriving the form of this functional is developed. The method of this derivation is based on the use of a nonlinear response theory. Our analysis shows that
G[
n] can be expressed entirely in terms of nonlinear response functions. We derive the full expression of
G[
n] which is written explicitly by the density
n(
r). Furthermore, we find the generalized form of “compressibility sum rule”.
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G. D. Goudaroulis, A. D. Jannussis
1974 Volume 36 Issue 2 Pages
386-392
Published: February 15, 1974
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In the present paper the Green-function of the lattice electron is calculated by use of the Wannier functions. Then the Green-functions of the free-electron in uniform fields are given and also the Green-function of the lattice electron in a uniform magnetic field, by considering the periodic potential as a perturbation, by use of the Schrauben functions.
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Masatoshi Nakayama
1974 Volume 36 Issue 2 Pages
393-398
Published: February 15, 1974
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A new type of surface mode of the electromagnetic wave is predicted in the case when charge carriers are located at the boundary of dielectric media. The dispersion relation of the mode is derived and its characteristic feature is discussed. Effect of the surface carrier is represented in terms of characteristic frequency
Ωs (=4π
Nse2⁄
m*c;
Ns is density of the surface carrier). The dispersion takes the linear form in the low frequency region (ω<<
Ωs), while it has the square root form (ω∝\sqrt
k) in the high frequency limit (ω>>
Ωs). In contrast to the case to the absence of surface carriers the present mode exists in the frequency region where at least one of the dielectric functions of the adjacent media takes positive value. As a numerical example the dispersion relation is calculated and illustrated for clean surface of
p-type InAs.
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Toshiyuki Ninomiya
1974 Volume 36 Issue 2 Pages
399-405
Published: February 15, 1974
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The frictional force acting on the dislocation is calculated for the fluttering mechanism based on the continuum approximation. It is shown that the equations of motion lead to the inelastic scattering of thermal phonons, resulting in transfer of their momentum to the dislocation. The frictional force by this mechanism has the T
3-dependence at low temperatures. If we use the Debye cut-off, the magnitude is about 1.6×10
−4 dyne·sec/cm
2 for Cu at room temperature.
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Kensuke Tani
1974 Volume 36 Issue 2 Pages
406-421
Published: February 15, 1974
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A phonon theory developed previously which is a new approach besides the self consistent phonon theory and which is generalization of the Born phonon theory giving the rigorous phonon frequencies and normal coordinates of a crystal at an arbitrary temperature, is applied to neutron scattering from lattice vibrations in an anharmonic crystal. This application is done using a moment expansion of the canonical correlation function in the form of a continued fraction. A displacive ferroelectric and a perovskite crystal which exhibits a structural phase transition are discussed in some detail. A magnetic system having the spin-phonon interaction due to modulation of the exchange interaction caused by lattice vibrations is also discussed. A scattering cross section which depends explicitly upon the interaction acting on a phonon and has an anomalous temperature dependence near the transition point is found in some cases.
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Kentaro Ohhashi, Ikuji Tsujikawa
1974 Volume 36 Issue 2 Pages
422-430
Published: February 15, 1974
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Magnetic properties of layered compounds of graphite, in which a FeCl
3 layer is separated by one (the 1st stage) or two layers (the 2nd stage) of graphite were studied by Mössbauer effect. The easy directions of spins were within the basal plane for the both stages, which were determined by measuring relative intensities of Zeeman components on samples of well orientated
c-axis. The temperature dependence of internal magnetic fields could be described according to the Weiss theory for
S=5⁄2 normalized to
Hn(0K)=500 kOe and with
TN=4 K. The coexistence of a central line and Zeeman lines, and their temperature dependent intensities could be interpreted as the superparamagnetic system with clusters of one molecular thickness and mean diameter ≈1000 Å. The observed quadrupole splittings 0.20 mm/sec for the 1st stage and 0.25 mm/sec for the 2nd stage were considered as due to trigonal distortions from the regular octahedrons of FeCl
3 molecule.
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Yuji Ito, Jun Akimitsu
1974 Volume 36 Issue 2 Pages
431-437
Published: February 15, 1974
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Magnetic from factor of Ni–Cr alloy with 4.5 at % Cr was measured by the polarized neutron diffraction method. From the form factor analysis, the mean localized moments of Ni and Cr were determined as 0.356±0.002 μ
B and 0.002±0.91 μ
B at room temperature respectively. The rate of decrease of the mean localized moment of Ni at 0 K with respect to the Cr concentration ∂μ
Ni⁄∂
c=−5.8±0.2μ
B is slightly steeper than that of the bulk moment. From this and from disturbance parameters of Cr in the Co
0.95Cr
0.05 alloy, the magnetic clusters around each environment dependent moment of Ni atoms in the Ni
0.95Cr
0.05 alloy were calculated.
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Takashi Yamaoka, Mamoru Mekata, Hideo Takaki
1974 Volume 36 Issue 2 Pages
438-444
Published: February 15, 1974
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Neutron diffraction was measured on single crystals of the disordered γ-phase Mn
1−xIr
x(
x=0.128, 0.170, 0.204 and 0.256). Diffraction patterns were interpreted by an antiferromagnetic two-sublattice structure with tetragonal symmetry. The (110) magnetic reflection was measured up to about 800 K for the determination of the temperature dependence of sublattice magnetization and the Néel temperature. The critical index for magnetization was found to be 0.38 for the
x=0.170 alloy. The Néel temperature increases remarkably with increasing Ir at a rate of about 9 K/at%Ir. The obtained magnetic form factors are well expressed by
f=(1⁄0.9)(
f3d−0.1
f4s) constructed from the scattering functions calculated by Freeman and Watson. The average magnetic moment per Mn atom increases from 2.2μ
B to 2.6μ
B with increasing Ir from
x=0 to
x=0.204. Diffuse scattering due to partial atomic order of Mn
3Ir was observed in the
x=0.256 alloys.
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Takashi Yamaoka
1974 Volume 36 Issue 2 Pages
445-450
Published: February 15, 1974
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Crystallographic and magnetic properties were studied in the disordered γ-phase Mn
1−xIr
x (0.05<
x<0.35) alloys. In Mn rich alloys, tetragonal distortion with axial ratio
c⁄
a>1 occurs at a temperature below their Néel temperature,
TN. The tetragonal distortion temperature,
Td in the antiferromagnetic ordered state decreases rapidly with increasing Ir and the alloys with
x>0.15 remain cubic down to low temperatures. On the other hand,
TN increases with alloying Ir at a rate of about 9 K/at%Ir up to 730 K at
x=0.25 and it is extrapolated to 500±20 K for fcc Mn. It was concluded that the anomalous rise of
TN is not mainly attributed to atomic order nor to the enhancement of exchange interaction due to lattice expansion, but that the perturbation of band structure due to alloying leads to stronger magnetic interaction. A Cu
3Au type atomic ordering in the vicinity of
x=0.25 was found to raise the
TN by about 200 K. The origin of tetragonal distortion is discussed.
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Tadashi Sugawara, Motoki Takano, Sigeru Takayanagi
1974 Volume 36 Issue 2 Pages
451-455
Published: February 15, 1974
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The resistivities of a series of dilute
MoMn,
MoFe and
MoCo alloys were measured between 1.5 K and room temperature in order to understand the nature of the s-d exchange interaction in these alloys. It was found that the resistivity of
MoCo and
MoFe shows a normal Kondo effect with a Kondo temperature of 46±2 K and about 0.3 K, respectively, while the resistivity of
MoMn shows a positive temperature coefficient with a characteristic temperature of 17±4 K, which is considered as the Kondo temperature of this alloy. In addition to these anomalies due to magnetic scattering, a peak was observed at about 50 K in the resistivity of all the alloys studied. This peak was attributed to the differing anisotropies of the relaxation times for impurity and phonon scattering.
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Mitsuo Kataoka
1974 Volume 36 Issue 2 Pages
456-463
Published: February 15, 1974
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The anomalous properties of Fe
2TiO
4, i.e. (i) the giant magnetostriction ((
c−
a)⁄
a=7.5×10
−3 at 77 K), (ii) the anomalously small elastic constant (
c11–
c12), and (iii) the positive magnetic anisotropy constant, are explained by taking into account both the Jahn-Teller effect of Fe
2+ ions in the
A-sites of the spinel structure and the spin-lattice coupling of Fe
2+ ions in the
B-sites. It is shown that when the direction of the Jahn-Teller distortion is determined so as to lower the energy of the coupling between the spins in the
B-sites and local distortions due to the Jahn-Teller effect, the Jahn-Teller distortion itself behaves as if it were a giant magnetostriction. The temperature dependences of the distortion, elastic constants and the specific heat are calculated. It is found that (
c11–
c12) has a minimum and the excess specific heat due to the Jahn-Teller ions has a maximum below the Néel temperature. Discussions on the magnetic anisotropy constant are also given.
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Osamu Sueoka
1974 Volume 36 Issue 2 Pages
464-469
Published: February 15, 1974
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Using the temperature dependence of the peak value in the angular correlation, the formation energy of a monovacancy in Cu and the effects of multivacancies on the peak value have been obtained. The formation energy of a monovacancy,
EF1v, is
EF1v=1.20±0.07 eV. The representation of the trapping model in plural trapped states has been given in the similar formulation to the conventional trapping model, was tried to apply for the data analysis.
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Toshihiko Taki, Tatsuo Kanashiro, Takashi Ohno, Mitsuo Satoh
1974 Volume 36 Issue 2 Pages
470-475
Published: February 15, 1974
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The nuclear magnetic double resonance technique has been used to study the first order quadrupole splittings of the NMR lines due to Na nuclei surrounding the substitutional impurities in NaCl single crystals. By studying the angular variation, signals observed are assigned to (0, 0, 1) Na sites around the Br
− impurities in NaCl–NaBr solid solutions, and to (0, 0, 1) Na and (1, 1, 1) Na sites close to the I
− impurities in NaCl–NaI crystal. The electric field gradients on these sites are found from the quadrupole frequency ν
Q obtained from our experiments and the nuclear quadrupole moment
Q=0.1×10
−24 cm
2 for Na nucleus:
eq=52×10
12 esu/cm
3 for (0, 0, 1) sites in NaCl–NaBr,
eq=140×10
12 esu/cm
3 for (0, 0, 1) sites and
eq=91×10
12 esu/cm
3 for (1, 1, 1) sites in NaCl–NaI.
The results are discussed in comparison with the theory considering the jonic displacements and the overlap of the electronic wave functions.
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Hiroto Kuroda, Shigeo Shionoya
1974 Volume 36 Issue 2 Pages
476-484
Published: February 15, 1974
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To study the dynamical processes of high density single excitons and excitonic molecules in CdSe, the time dependences of M, P
M and P luminescence lines and the time-resolved absorption spectra of A excitons are measured in the pico-second region at 4.2 K. The exciton absorption peak shifts to the high energy side due to the high density effect, the shift reaching the maximum at 20 ps after the pulse excitation. M line reaches the maximum at 100 ps, P
M line at 200 ps and P line at 300∼350 ps. The decay constants are 100, 100 and 350 ps, respectively. The dynamical aspects of the formation of A excitons, the formation of excitonic molecules and the inelastic collisions of single excitons and excitonic molecules are discussed. It is interpreted why the use of the pico-second pulse excitation is essentially important for the realization of the Bose condensation of excitonic molecules.
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Hajime Hattori, Osamu Fujitani, Masayoshi Umeno
1974 Volume 36 Issue 2 Pages
485-490
Published: February 15, 1974
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The second (μ-type) photoconductive effect due to the inter-valence band transition of germanium was observed during the experiment on the photon drag effect. In order to discuss this effect, an analysis was done under the assumption that the heavy and light holes are relaxed by the intra-band and inter-valence band transitions, respectively. The result shows that the photoconductivity depends most strongly on the heavy hole density. The theoretical predictions on the temperature dependence of photoconductivity were in good agreement with the experiment.
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Tatsumi Kurosawa, Hajime Maeda, Hidehiko Sugimoto
1974 Volume 36 Issue 2 Pages
491-497
Published: February 15, 1974
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Hot carrier instability associated with the negative differential conductivity in a transverse magnetic field is discussed with emphasis on its marked differences from the instability when not under the magnetic field. The condition for the instability is considerably changed by the presence of the magnetic field, because the current is not parallel to the electric field and the negative differential conductivity has to be defined differently from the usual case. Generally, a system in the magnetic field becomes unstable more easily than a system not in the magnetic field does. Under a strong magnetic field, even a weak non-linearity in the current-field characteristic sometimes can bring about the instability. The domain structure expected in the present case and experimental facts relevant to the present theory are also discussed.
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Hiroyasu Shimizu, Makoto Tsukamoto, Yoshihiro Ishibashi, Masayoshi Ume ...
1974 Volume 36 Issue 2 Pages
498-503
Published: February 15, 1974
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The Brillouin scattering spectra in NaNO
2 have been studied using a Fabry-Perot interferometer. The observed Brillouin shifts for eighteen acoustic phonons in nine scattering geometries have been assigned to specific modes of vibration. The determined values of nine elastic constants in units of 10
10 dyn/cm
2 are
C11=31.7,
C22=58.2,
C33=66.0,
C44=12.4,
C55=9.91,
C66=4.79 (
C66D=4.98),
C12=12.6,
C23=17.4 and
C13=19.7 at room temperature. The temperature dependence of
C22D associated with the longitudinal phonon propagating along the ferroelectric
b-axis has been studied with particular emphasis in the region close to the Curie and the Néel points. The elastic stiffness constant
C22D showed anomalous decrease both at the Curie and the Néel temperatures. These results are compared with those obtained in the ultrasonic region.
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Eiichiro Nakazawa, Shigeo Shionoya
1974 Volume 36 Issue 2 Pages
504-510
Published: February 15, 1974
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Rather sharp zero-phonon lines accompanied by many vibronic lines are observed in the near-ultraviolet luminescence and excitation spectra due to the 4f-5d transitions of Ce
3+ ion in YPO
4 and LuPO
4 crystals at low temperature. Comparing the vibrational energies of the vibronic lines with the results of infrared and Raman measurements of YPO
4 crystals, it is shown that these vibronic lines can be separated into two parts; the one is due to the lattice (external) vibration of Y
3+ and PO
43− ions and the other is due to the coupled molecular (internal) vibration of PO
4 complexes. The coupling scheme of these vibrations with the 4f or 5d electron of Ce
3+ ion is discussed.
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Hitoshi Kanamori, Shinji Hayashi, Yasukazu Ikeda
1974 Volume 36 Issue 2 Pages
511-516
Published: February 15, 1974
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All the symmetry coordinates for long-wavelength lattice vibration, external modes 2B
g+2E
g+2A
u+2E
u and internal modes 3A
g+3B
g+3E
g+3A
u+3B
u+3E
u, are obtained by the group theoretical calculations including the projection operator technique. For internal modes, site symmetry consideration simplifies the procedure. For external modes, two possible sets of force constants between first and second neighbour ions in CaWO
4, CaMoO
4 and SrMoO
4 are obtained from Raman and infrared frequencies. Normal coordinates are derived and briefly schematized.
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Hisao Hagiwara, Ryozo Oyamada
1974 Volume 36 Issue 2 Pages
517-522
Published: February 15, 1974
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Four characteristics of the glassy PbO–GeO
2 system were examined. X-ray diffraction pattern of the sample of 50 mol % PbO showed the maximum intensity at
d-value 2.885 Å which was in accordance with that of the compound PbO·GeO
2 (relative intensity 60 %). Infrared absorption band of the glassy GeO
2 at 11.5 μ, which would be assigned as ν
3 mode of tetrahedral GeO
4 unit, shifted toward longer wavelength side with increasing PbO content and the shift showed a plateau at 47–50 mol % PbO. Dielectric constant also kept nearly constant value at 47–50 mol % PbO. The wavelengths corresponding to the intrinsic absorption coefficients per PbO mole fraction (
e. g. 70 cm
−1/m.f.) increase linearly with increasing PbO content, having the inflection point at 45 and 55 mol % PbO. The ionic character of the bond GeO
4–Pb is discussed on the basis of the results.
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Nobuo Tsuda, Takefumi Mitsuhashi, Toshinobu Chiba
1974 Volume 36 Issue 2 Pages
523-525
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Angular correlation curve of powdered monoclinic ZrO
2 was taken and compared with some calculated curves, It is expected that the wave function of oxygen 2s electron extends more outwards than that used here.
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Yutaka Kano
1974 Volume 36 Issue 2 Pages
526-528
Published: February 15, 1974
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The optical equivalence theorem is examined for the particular class of the electromagnetic fields. It is shown that the distribution function can be taken as a non-negative function, if the density operator describing the states of the electromagnetic field is diagonal in the occupation number representation. Hence the equivalence is not only formal but also essential for this class of the electromagnetic fields, so long as the description of the optical coherence theory is concerned. As a typical example the “diagonal” representation of the density operator for blackbody radiation is studied.
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Osamu Saito, Tsuneto Takahashi
1974 Volume 36 Issue 2 Pages
529-531
Published: February 15, 1974
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A relation between the number of intra-molecular linkages created in amorphous polymers by cross-linking reaction and the second moment of molecular size distribution is obtained. It is shown by comparing the relation with the results of Monte Carlo calculation that the theory gives a good estimation of the number of intra-molecular linkages, which is negligible up to the point.
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Hiroshi Asai
1974 Volume 36 Issue 2 Pages
532-536
Published: February 15, 1974
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Electric birefringence and electric dichroism methods are proposed, which can decide the most plausible transition model for a given allosteric protein. Asymmetric quarternary conformations which appear at an intermediate concentration of ligand in the case of the KNF model or a more generalized model can be detected directly by the appearance of electric permanent dipole in birefringence of dichroism. A theorem concerning the maximum concentrations of asymmetric quarternary conformations is also derived, and suggested to be useful for evaluation of various thermodynamic parameters in transition models.
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Seiji Tsurubuchi, Tsuruji Iwai, Tadao Horie
1974 Volume 36 Issue 2 Pages
537-541
Published: February 15, 1974
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Absolute measurements of the emission cross-sections for the
A-
X band-spectrum of OH and the
Hβ line in the dissociative excitation processes of H
2O by electron-impact have been carried out by means of the crossed-beam technique, with the aid of a high sensitive spring balance made of fused quartz. The spring has a tiny pan, which is surrounded by a specially designed trap of liquid nitrogen. The spring words well for direct intensity measurements of the water molecular beam, because the condensation coefficient of H
2O on ice is large enough at lower temperatures.
The following results have been obtained; (4.2±2.1)×10
−18 cm
2 for the
Hβ transition, and (7.1±3.5)×10
−18 cm
2 for the OH (
A,
2Σ+−
X,
2Π) transition, at 300 eV respectively.
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Kiyoji Uehara, Koichi Shimoda
1974 Volume 36 Issue 2 Pages
542-551
Published: February 15, 1974
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The magnetic hyperfine interactions in the triply degenerate vibrational state of
12CH
4 are theoretically studied. The spin-vibration interaction is introduced as well as the spin-spin and spin-rotation interactions to obtain the explicit expressions of matrix elements of the hyperfine energy. The numerical calculations are carried out for the 6
7 F1(2) and
A1 sublevels in the
v3=1 exited state and a comparison is made with a recent measurement of Hall and Bordé on the
F1(2) line.
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S. K. Kor, N. D. Tripathi
1974 Volume 36 Issue 2 Pages
552-554
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Assuming the atomic motions in water, methanol and ethanol as similar to those of solids, the effective Debye temperature has been calculated as a function of temperature and pressure for these liquids.
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Michiru Yasuhara, Kenji Yoneda, Susumu Sato
1974 Volume 36 Issue 2 Pages
555-557
Published: February 15, 1974
Released on J-STAGE: May 29, 2007
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Vibrational relaxation time τ of a gaseous methane behind shock waves at pressure
p, are measured from the density variation obtained by using a narrow beam laser schlieren method. The results obtained for a temperature range of
T=300–800 K are shown in a Landau-Teller plot, which shows essentially the linearity of ln
pτ versus
T−1⁄3. Also the results obtained by the ultrasonic method are shown to give a good comparison with the present method.
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Kozaburo Tamura, Junichi Fukushima, Hirohisa Endo, Shigeru Minomura, O ...
1974 Volume 36 Issue 2 Pages
558-564
Published: February 15, 1974
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The effect of pressure on the electrical resistance of amorphous Ge and Ge–Sn alloys prepared by the evaporation onto mica substrates has been measured up to about 130 kbar. It is found that the semiconductor to metal transition occurs at pressure of 60 kbar in amorphous Ge, and this transition pressure is changed by alloying of Sn.
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Kozaburo Tamura, Junichi Fukushima, Hirohisa Endo, Kosaku Kishi, Shige ...
1974 Volume 36 Issue 2 Pages
565-571
Published: February 15, 1974
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X-ray photoelectron emission spectra for the amorphous binary alloys between Ge and Ni, Fe and Au have been obtained. The positions and shapes of the main peaks associated with d-band of Ni, Fe and Au in the spectra change with addition of Ge. The valence orbitals of s and p symmetries of Ge in Ni, Fe and Au may mix with the s, p and d-orbitals of surrounding host atoms to form bonding and antibonding molecular orbitals.
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Kunizo Ohkubo, Shigetoshi Tanaka
1974 Volume 36 Issue 2 Pages
572-578
Published: February 15, 1974
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By means of the probe antenna, the electrostatic wave in the low density region and the Whistler wave in the high density region can be excited in the magnetized plasma column with the finite diameter. The propagation characteristics of both waves are measured in detail by the interferometer method. The observed transition region from the electrostatic to Whistler wave is interpreted well by using the model of the longitudinally magnetized plasma waveguide. It is experimentally confirmed that the Whistler wave is right-hand circularly polarized. The observed dispersion curves agree well with theoretical prediction.
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Masashi Kando, Susumu Takeda
1974 Volume 36 Issue 2 Pages
579-584
Published: February 15, 1974
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The diffusion waves in a plasma are analyzed for the ion-neutral collision frequency greater than the ion plasma frequency. It is, then, observed that with the increase in frequency, the diffusion wave tends to a mode governed by an electron free diffusion rather than the ion acoustic mode. The experiment has been mode in an axially decaying helium plasma produced by r.f. discharge at the pressures of 2.0 and 4.0 Torr. The interferometer patterns of the diffusion waves are well explained by the theory proposed here.
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Shobu Kaneko, Toshihide Tsunematsu
1974 Volume 36 Issue 2 Pages
585-590
Published: February 15, 1974
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The hydromagnetic energy principle is applied to the derivation of the necessary and sufficient condition for the stability of the linear Bennett pinch. Two models of the finite-radius pinch are considered. In the first model, the radius of the plasma column is assumed to be equal to the radius of a conducive wall. In another model, the radius of the plasma column is assumed to be smaller than the radius of the wall. Though long-wavelength kink disturbances are stabilized by the conductive wall, the stability conditions of both models for all kink disturbances change only slightly from the stability condition of an infinite-radius pinch. Sausage disturbances are stabilized more effectively by the wall. It is shown that the conductive wall has little effect on the stability of the pinch in the Tokamak device if it can be represented by the Bennett pinch.
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Yukiharu Ohsawa, Kazuhiro Nozaki
1974 Volume 36 Issue 2 Pages
591-595
Published: February 15, 1974
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New solutions of solitary pulses in three-wave interactions are obtained, which were not given in the previous paper of this series. In those solutions, the wave of lower frequency has a shock-type envelope and behaves as a “pump” while the other two waves have the pulse-type ones. In addition, by considering two effects, linear translations of the waves and nonlinear interactions, a physical mechanism of formation of the solitary pulses is found. The theory is applied to the interaction among two Alfvén waves and an ion-acoustic wave, which propagate along the external magnetic field.
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Toshio Tange
1974 Volume 36 Issue 2 Pages
596-602
Published: February 15, 1974
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The dielectric response function of a two-component, inhomogeneous plasma in a magnetic field is calculated from a solution of the Vlasov equation, to the first-order terms in the density-gradient expansion. The spectral function of the electric-field fluctuations is then obtained with the aid of the superposition principle of the dressed test particles. The physical interpretation of the results is given in terms of the effects arising from the spatial variation of the average density and those created by the diamagnetic drift.
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Setsuo Ichimaru, Toshio Tange
1974 Volume 36 Issue 2 Pages
603-609
Published: February 15, 1974
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The diffusion coefficient of the electrons across a magnetic field (with strength
B) is calculated in terms of the spectral function of the electric field fluctuations. The calculation is based on the microscopic evaluations of the first and second moments of the guiding-center displacements under the action of the fluctuating electric field in an inhomogeneous plasma. For a Maxwellian plasma, it is found that the diffusion coefficient contains an anomalous term D
⊥* in addition to the usual classical term; D
⊥* is proportional to
B−1 when ω
e2(1+
Te⁄
Ti)>>
Ωe2, and to
B−2ln
B when ω
e2(1+
Te⁄
Ti)<<
Ωe2, where ω
e is the electron plasma frequency, and
Ωe, the electron cyclotron frequency. The contributions of the like-particle interactions vanish identically in the idiffusion coefficient.
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Akira Sakurai
1974 Volume 36 Issue 2 Pages
610
Published: February 15, 1974
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Kôki Ikeda, Takurô Nakamichi, Tutomu Yamada, Mikio Yamamot ...
1974 Volume 36 Issue 2 Pages
611
Published: February 15, 1974
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Tokiyoshi Itagaki, Takao Karakizawa, Shoichi Shiina, Haruyuki Ohonishi ...
1974 Volume 36 Issue 2 Pages
612
Published: February 15, 1974
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Michio Kiritani, Naoaki Yoshida
1974 Volume 36 Issue 2 Pages
613
Published: February 15, 1974
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Hiroshi Kameyama, Yoshihiro Ishibashi, Yutaka Takagi
1974 Volume 36 Issue 2 Pages
614
Published: February 15, 1974
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J. Geiger
1974 Volume 36 Issue 2 Pages
615
Published: February 15, 1974
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