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Kazu Nishigaki
1982 Volume 51 Issue 6 Pages
1703-1704
Published: June 15, 1982
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It is shown that the scaled superheat-limits for variety of liquids including neon—its superheating was observed in this work, are approximately represented by a simple universal function as (
Tnucleation−
Tcoext)⁄
Tcritical\simeq0.68(
Tcritical−
Tcoext)⁄
Tcritical, and that the empirical result can be explained in terms of a modified version of the Döring-Zeldovich-like nucleation theory by Langer and Turski.
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Hideki Miyajima
1982 Volume 51 Issue 6 Pages
1705-1706
Published: June 15, 1982
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Magnetic field dependence of the magnetic susceptibility of Iron-Monosilicide FeSi was measured to investigate the mode-mode coupling for spin fluctuations. The susceptibility increases with magnetic field, and straight lines in Arrott plots have negative slope. These results suggest that mode-mode coupling for spin fluctuations is negative. This fact is in substantial agreernent with theoretical predictions proposed by Takahashi and Moriya on the basis of a unified picture of itinerant electron magnetism.
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Masasi Inoue, Kazutoshi Fukui, Hisao Yagi, Toshiaki Tatsukawa
1982 Volume 51 Issue 6 Pages
1707-1708
Published: June 15, 1982
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A modified mutual inductance bridge has been used to measure ac magnetic susceptibility χ (frequency 155 Hz and intensity 8 Oe) of degenerate magnetic semiconductors Sn
1−xMn
xTe (
x=1 at.%, 3 at.%, and 5 at.%) at liquid He temperatures. In contrast to the high-field (5 kOe) susceptibility data, the low-field susceptibility shows two magnetic transitions at the characteristic temperatures of
TAHE (5–6 K) and
Tm (4–5 K).
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Hidetoshi Fukuyama
1982 Volume 51 Issue 6 Pages
1709-1710
Published: June 15, 1982
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It is pointed out that the excitonic superconductivity proposed by Little will be possible along dislocations, since metallic linear paths can be formed, as the case may be, along dislocations in otherwise semiconducting (or insulating) bulk materials.
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Atsuo Matsui, Hitoshi Nishimura
1982 Volume 51 Issue 6 Pages
1711-1712
Published: June 15, 1982
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Based on the observation of free exciton luminescence at room temperature, self trapping of excitons is recognized in β-perylene crystals which have a monomeric structure. Temperature dependence of the luminescence spectra suggests the existence of two sorts of self trapped states. The result obtained are consistent with those anticipated by the analysis of the Urbach rule in β-perylene.
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Ichiro Fujiwara, Nobutsugu Imanishi, Tomota Nishi
1982 Volume 51 Issue 6 Pages
1713-1719
Published: June 15, 1982
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The independent isomer-yields of
132I(4
+, 8
−),
134I(4
+, 8
−),
135Xe(3/2
+, 11/2
−) and
138Cs(3
−, 6
−) have been measured in the thermal-neutron induced fission of
233U,
235U and
239Pu. From the isomer-yield ratios, the mean angular momenta of the primary fragements have been deduced on the basis of thc statistical analysis. Obtained results indicate that the primary angular momentum 〈
J〉h is higher in odd-
Z products than in even-
Z ones, and increases up to a certain value at an approximate rate of −
Δ〈
J〉⁄
Δ(δ
N)∼0.8 h with decreasing neutron displacements δ
N, which is defined as the difference between the number of neutron
N in the products and the most probable neutron number
Np in the isotopic yield distribution.
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Toshihico Arimitsu
1982 Volume 51 Issue 6 Pages
1720-1726
Published: June 15, 1982
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General formulation for open systems is given in terms of the time-convolution-less formulation of the damping theory. A diagramatic construction rule for the “kinetic coefficient” is given by introducing the mirror operation of the time evolution operator. The response function generalized to the open systems is derived by using the general formulation. Formally, the response function can be written in the same form as was given by Kubo by using the mirror commutator instead of the conventional one.
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Yoko Hamano, Fumiaki Shibata
1982 Volume 51 Issue 6 Pages
1727-1736
Published: June 15, 1982
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Our previous theory of spin relaxation is extended to determine appropriate solutions for general cases without the narrowing condition. This is done by means of a consistent use of the projection operator formalism. The basic equation thus derived can be used for any time-scale.
Explicit solution is obtained for
J=1⁄2 (
J the magnitude of spin); there exists a correspondence between our quantum mechanical theory and a stochastic theory.
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Isao Harada, Akio Kotani
1982 Volume 51 Issue 6 Pages
1737-1744
Published: June 15, 1982
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Commensurate and incommensurate states of a Heisenberg spin-Peierls system in a magnetic field are studied within the mean-field approximation. Free energy, order parameter and magnetization are calculated numerically by taking account of the effect of all the accompanying harmonics. In particular, it is found that at low temperatures the field lowers the free energy of the incommensurate states and results in the commensurate to incommensurate phase transition. The nature of this transition is discussed. It is also found that the incommensurate to normal phase transition temperature behaves anomalously in a strong field. The resultant phase diagram is compared with the experimental data on TTF–CuBDT.
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Hitoshi Sumi
1982 Volume 51 Issue 6 Pages
1745-1762
Published: June 15, 1982
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Energy transfer (ET) is greatly enhanced in a very short time after the initial electronic state was prepared by photon excitation. ET is assisted by violent lattice vibrations which have not been relaxed yet, when electrons interact strongly with phonons in the two electronic states (coupled by the matrix element
J). An expression of the quantum yield of ET, which bridges the nonadiabatic (small
J) and the adiabatic (large
J) limits, is given as a function of time elapsed after pulsed excitation at an energy
E. In the case of steady excitation, transitions during vibrational relaxation manifest themselves in a strong
E dependence of the quantum yield. Generalization of Förster’s formula for ET in this dynamic regime is also mentioned. We use a formulation developed in the part I (J. Phys. Soc. Jpn.
49 (1980) 1701) which treat transitions after vibrational relaxation. The Landau-Zener formula plays an important role in describing ET.
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Kenichi Nanbu
1982 Volume 51 Issue 6 Pages
1763-1768
Published: June 15, 1982
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Molecular boundary conditions has a crucial effect on the correlation of velocity between two molecules. First, the effect is analysed by using a stochastic model for molecular reflection at the wall; the model is a combination of specular and diffuse reflection. As the percentage ζ
D of diffuse reflection increases, the correlation coefficient ρ drastically decreases; it is at most of order (ζ
DN)
−1,
N being the number of simulated molecules. Next, the effect is examined by analysing the data from actual simulation calculations. The behavior of the data is consistent with the magnitude of ρ determined by using the reflection model. If ρ is less than about 3%, the simulation data for any boundary conditions are essentially the exact solutions of the Boltzmann equation.
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Hiroaki Kato, Motohiko Yamada, Hiroshi Yamauchi, Hidetoshi Hiroyoshi, ...
1982 Volume 51 Issue 6 Pages
1769-1777
Published: June 15, 1982
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Magnetic susceptibilities and magnetization isotherms have been measured for single crystal FeTiO
3. The susceptibility parallcl to the
c-axis has a large and sharp peak at
TN=58.0±0.3 K, while the perpendicular susceptibility is almost independent of temperature below
TN. Magnetization isotherm at 4.2 K with fields applied along the
c-axis exhibits a typical metamagnetic transition at
Hc=80.3±0.1 kOe, being the first observation of metamagnetism in 3
d transition metal oxides. The transition is of the first order up to about 35 K, above which it is of the second order. The experimental data are well reproduced by molecular field calculations with the best fit parameters of the anisotropy field
HA=150 kOe, the ferromagnetic intrasublattice exchange interaction of 2
z1J1=28.5 K, and the antiferromagnetic intersublattice interaction of 2
z2J2=−6.67 K.
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A. H. Nayyar
1982 Volume 51 Issue 6 Pages
1778-1784
Published: June 15, 1982
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It is shown that in a hyperfine coupled system of nuclear and helically ordered electronic spins, an external magnetic field destroys the otherwise necessarily occuring zero-energy (Goldstone) mode, provided the external field is of the order of the hyperfine field. It is argued that the applied field acts against the internal hyperfine field in a manner such as to prevent the nuclear spins from following the electronic spins and thereby destroys the degeneracy of the ground state. Numerical calculations of the excitation energies of the coupled system for Holmium metal, as an example, are presented to show this conclusion explicitly.
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Hiroshi Mori, Takeo Satoh, Haruhiko Suzuki, Taiichiro Ohtsuka
1982 Volume 51 Issue 6 Pages
1785-1791
Published: June 15, 1982
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Heat capacity data are presented for intermetallic compounds PrNi
2, YNi
2 and the pseudobinary system Pr
cLa
1−cNi
2. The temperature range covered is 2 to 80 K. The magnetic heat capacity deduced under certain assumptions shows that in PrNi
2 the singlet
Γ1 is the ground level and that the first excited level lies about 60 K above the ground level. An excess contribution is found around 10 K. The excess heat capacity is understood if the excited level is assumed to have appreciable broadening due to the exchange interaction acting between Pr atoms.
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Yoshinori Takahashi, Michiyasu Tano
1982 Volume 51 Issue 6 Pages
1792-1798
Published: June 15, 1982
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The metamagnetism in the ground state and magnetic susceptibilities of Co(S
xSe
1−x)
2 at finite temperature are discussed based on the recent spin fluctuation theory of Moriya-Takahashi. The critical field for the metamagnetic transition, the critical temperature, and the temperature dependence of the magnetic susceptibility are qualitatively and semi-quantitatively explained consistently with the use of the model density of state derived from the recent band structure calculation by Asano.
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Ze Xianyu, Yoshikazu Ishikawa, Shigehumi Onodera
1982 Volume 51 Issue 6 Pages
1799-1803
Published: June 15, 1982
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The spin wave excitation has been studied by both inelastic neutron scattering and magnetization measurement for the amorphous Fe
70Cr
10P
13C
7 alloy which almost does not exhibit the invar properties. Well defined magnon groups have been detected around (0, 0, 0) at up to
q=0.16 Å
−1 for various temperatures below
T≤0.9
Tc. The spin wave stiffness constant
Ds has been determined to be
Ds=60±2 meVÅ
2 by neutron scattering which is nearly in agreement with the value
Dm=54±2 meVÅ
2 derived by the magnetization measurement. The spin wave linewidth
Γ varies with both wave vector
q and temperature
T as
Γ∝
q4T2 as predicted for the two-magnon interaction in the Heisenberg system.
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Ryohei Nakata, Katsuyasu Kawano, Minoru Sumita, Eiichi Higuchi
1982 Volume 51 Issue 6 Pages
1804-1810
Published: June 15, 1982
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The line positions and intensities of the ESR from Eu
2+ ions in SrF
2 crystals have been investigated at room temperature and at 9.5 GHz. A perturbation calculation gives satisfactory results in their angular dependences when cross terms between the cubic crystal field (
b4⁄60)·(
O40+5
O44) and the hyperfine terms
AiS·
Ii are taken into account. The relative sign of
b4 and
Ai can be determined from the angular dependence of the doublet separations in the forbidden transitions.
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Nobuko Sakai, Ken-ichi Takemura, Kazuhiko Tsuji
1982 Volume 51 Issue 6 Pages
1811-1816
Published: June 15, 1982
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The electrical resistance up to 250 kbar and down to 1.7 K, and the thermoelectric power up to 250 kbar at room temperature have been measured in iodine using a diamond-anvil cell. The resistance decreases rapidly and continuously with increasing pressure. The resistance anomaly has been found at 225 kbar and room temperature. The resistive characteristic temperature θ in the Grüneisen-Bloch equation is 225 K for metallic iodine at 235 kbar. The thermoelectric power decreases from a large positive value to a small positive one with increasing pressure and is +4±3 μV/deg at 240 kbar. These electrical properties have been discussed in relation to the structural change induced by pressure.
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Keizo Murata, Takashi Ukachi, Hiroyuki Anzai, Gunzi Saito, Koji Kajimu ...
1982 Volume 51 Issue 6 Pages
1817-1825
Published: June 15, 1982
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Two types of nonlinear effects in the electrical conductivity along the most conductive
a-axis of (TMTSF)
2ClO
4 were observed near the superconducting transition temperature. Along the
a-axis, the resistivity decreased as decreasing the temperature between 300 K and 5.5 K and turned to increase down to 1.07 K below which the superconductivity appeared. One of the nonlinearities was the increase in resistance up to a value greater than the normal one at a current just above the superconducting critical current. Along the
c*-axis, the least conductive axis, such nonlinearity was not observed. The other is the decrease in resistance driven by the current much larger than the critical current, which seems to show the restoration of the metallic behavior. The influences of thermally induced microcracks on the temperature dependence of resistivity and to the nonlinearities are also presented.
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Akio Yoshimori, Jean-Loup Motchane
1982 Volume 51 Issue 6 Pages
1826-1833
Published: June 15, 1982
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The friction coefficient, η, of chemisorbed atoms on metal surfaces, originating from electronic fluctuation, is discussed on the Newns-Anderson model. Emphasis is put on the effects of electron correlation on the adatom, the resulting temperature dependence and position dependence of η. The Ward identity is found to be useful in deriving the compact expression for η in terms of the phase shift. An anomalous temperature dependence of the surface diffusion coefficient is shown as a possible example to examine the effect of η. Discussion is given on a relation between the expression of η and the “excess resistivity”, which is also related to the electromigration problem in bulk.
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Tsuneaki Miyahara, Hiroyoshi Ishii, Takaaki Hanyu, Haruo Ohkuma, Shige ...
1982 Volume 51 Issue 6 Pages
1834-1839
Published: June 15, 1982
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Optical absorption coefficients of La, Ce, Sm, Eu and Gd metals have been measured in the photon energy range from 6 to 40 eV. Contribution of the 4
f electrons to the optical absorption has not been observed in the present photon energy region. The 5
p threshold of Ce, Sm, Eu and Gd does not show sharp absorption edge. The rounded edge indicates that the size of the 5
p core hole should be larger than that in heavy simple alkali metals.
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Yasuo Nozue
1982 Volume 51 Issue 6 Pages
1840-1850
Published: June 15, 1982
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Dispersion relations of the multicomponent Z
1,2 exciton-polaritons for
K⁄⁄[111] and
K⁄⁄[110] are determined by the two-photon-resonant Raman scattering via the excitonic molecule state, and there appears the significant anisotropy between them. These polariton dispersions are self-consistently analyzed by the theoretical forms of the symmetry-breaking effect due to a finite wave vector, where the
K-linear, the heavy- and light-mass, and the warping effects are confirmed. The effective mass of the lowest molecular state is determined.
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Kazutaka Tsuji, Shuzo Takano
1982 Volume 51 Issue 6 Pages
1851-1856
Published: June 15, 1982
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Quantum oscillations of shear acoustic wave were observed in
p-Pb
1−xGe
xTe (
x=0.014) at liq. He temperatures. Three kinds of different branches of the frequencies were resolved by the Fourier analyses of the oscillations. By comparing with the theoretical model of the energy surfaces by Takaoka and Murase, these oscillations were identified as arising from the triplet up-, the triplet down- and the singlet down-state energy surfaces. The singlet up- energy surface is too small to be observed. From the ratios of the observed frequencies for magnetic field parallel to the major axis of the energy surfaces, we estimated
ΔEv=0.006 eV and
Ξu=0.06 eV where
ΔEv is the downward shift of the valence band edge at L-point relative to that at T-point,
Ξ is the optical deformation potential constant and
u is the internal displacement of the sublattices.
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Sadao Takaoka, Kazuo Murase
1982 Volume 51 Issue 6 Pages
1857-1864
Published: June 15, 1982
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The band edge structure modification of Pb
1−xGe
xTe due to the structural phase transition has been investigated by means of the interband absorption and the Shubnikov-de Haas (SdH) effect. Below the phase transition temperautre (
Tc) the band gap determined by the optical absorption increases with lowering temperatures or at least its temperature coefficient changes. From the SdH effect below
Tc, we obtained the information of the carrier redistribution among the conduction (or valence) bands caused by the phase transition.
These results can be explained only when we take into account the effects of relative sublattice displacement and the homogeneous strain at the same time.
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Michihide Kitamura, Hirogi Iwata, Toshihiro Arai
1982 Volume 51 Issue 6 Pages
1865-1870
Published: June 15, 1982
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The optical absorption spectrum, D.C. conductivity, thermoelectric power and infrared (I.R.) reflection spectrum have been measured for (As
2Se
3)
100−xGe
x (
x=0, 1, 5, 10) glasses. The optical absorption coefficient were analyzed on the basis of the model proposed by Kolobov and Konstantinov and the D.C. conductivity and the thermoelectric power were analyzed on the basis of the model proposed by Emin. The adiabatic potentials of these materials were calculated from these results. We might conclude that the square of the electron-phonon coupling strength is directly proportional to the curvature of the adiabatic potential and that the proportional constant is approximately equal to the optical gap,
Eopt, obtained experimentally.
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Atsuo Matsui, Kenichi Mizuno, Motoaki Iemura
1982 Volume 51 Issue 6 Pages
1871-1877
Published: June 15, 1982
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The shape of the lowest exciton absorption band in α- and β-perylene due to the B
2u←A
g transition, the halfwidth of the absorption band, and the steepness parameter of the Urbach tail are investigated. From linear temperature dependence of the halfwidth and the Lorentzian line-shape, the transition A
u←A
g is well explained by the exciton band picture. The lattice relaxation behavior of excitons after they are formed is described by the strong exciton-phonon coupling scheme.
Based on the steepness parameter obtained, 0.93 in α-perylene and 1.38 in β-perylene, and the amount of the Davydov splitting obtained, 2040 cm
−1 in α-perylene and 960 cm
−1 in β-perylene, the lattice relaxation energy is estimated to be 1530 cm
−1 and 523 cm
−1 respectively. Also the energy difference between the free and self-trapped exciton states is expected to be 620 cm
−1 in α-perylene and 43 cm
−1 in β-perylene.
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Hirokazu Tanaka, Itaru Tatsuzaki
1982 Volume 51 Issue 6 Pages
1878-1883
Published: June 15, 1982
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Linewidths of the acoustic phonons propagated and polarized in the
ab plane were measured for various scattering angles between π⁄6 and 5π⁄6 by the use of 4880 Å light. It was observed that the linewidths of the quasitransverse waves broaden as the temperature is lowered to the transition point; the linewidths of these phonon peaks depend not only on the direction, but also on the magnitude of their wave vectors. These results are discussed by taking into account of the piezoelectric interaction between the
xy shear component of the acoustic phonons and the
z-component of the polarization fluctuation.
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Saburo Yokota
1982 Volume 51 Issue 6 Pages
1884-1891
Published: June 15, 1982
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Optical and X-ray examinations of CsHSeO
4 were made above and below the phase transition point (
Tc). CsHSeO
4 undergoes an improper ferroelastic phase transition at 128°C and has spontaneous strains
e130=2.7×10
−2 and (
e220−
e110)⁄2=7.9×10
−2 at room temperature. The crystal is tetragonal above
Tc with the unit cell parameters
at=
bt=4.18 Å and
ct=7.20 Å at 130°C, and exhibits a superlattice structure with the monoclinic unit cell parameters
am\simeq2
at and
bm\simeq2
bt below
Tc. It is shown that if we assume 4⁄
mmm as the point group above
Tc, all the domain structures observed in CsHSeO
4 below
Tc, which disappear above
Tc, can be deduced from the strain-compatibility relations for domain boundaries by taking account of the symmetry change from 4⁄
mmm to 2⁄
m associated with the phase transition.
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Hakaru Yamanaka, Masanori Hangyo, Yoshihiro Hishikawa, Riso Kato
1982 Volume 51 Issue 6 Pages
1892-1899
Published: June 15, 1982
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It has been found that the peculiar lines A, B, C, D and E which appear in the spectrum of the singlet luminescence in NaNO
2 crystal are strongly enhanced when the crystal is doped with NO
3− impurity. A number of sharp lines on the tail of the zero-phonon line of the singlet absorption in the crystal are also enhanced by NO
3− impurity. From the excitation spectra for the luminescence lines, it is shown that both luminescence and absorption lines have common origins. They are interpreted as the lines due to the transition (
Remark: Graphics omitted.) in NO
2− ions which are perturbed by the presence of NO
3− impurity in the crystal.
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Ko Sugihara, Shusuke Ono, Hisashi Oshima, Kiyoshi Kawamura, Takuro Tsu ...
1982 Volume 51 Issue 6 Pages
1900-1903
Published: June 15, 1982
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Low field Hall coefficient
R in well-crystalline graphite is positive at low temperatures.
R reveals a maximum around 0.2 kOe at low temperatures and decreases rapidly with
H→0. This trend can not be eplained without invoking the trigonal warping of the bands. The trigonal warping appreciably modifies the electron bands, and the harmonics induced by the trigonal warping corresponds to the appearance of the small effective mass carriers. This effect predominates over the contribution due to the holes around
H-point. An exact calculation of
R (
H→0) is carried out for γ
3=0.29 eV, and the comparison with our measurements (I. Experimental) is performed.
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Atsushi Kurobe, Hiroshi Kamimura
1982 Volume 51 Issue 6 Pages
1904-1913
Published: June 15, 1982
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Effects of intra-state correlation on the variable range hopping are investigated in the absence and presence of a magnetic field. In the absence of a magnetic field, Mott’s expression for the resistivity, ρ∝exp [
T0⁄
T]
1⁄4, still holds in its temperature dependence. However, the prefactor
T0 now depends on two types of localization lengths brought about by the intra-state correlation. Magnetoresistance is found to be positive due to the intra-state correlation. It shows a linear dependence on a magnetic field in lower magnetic fields and saturates above a certain magnetic field.
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Wilhelm Brenig
1982 Volume 51 Issue 6 Pages
1914-1920
Published: June 15, 1982
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Nonadiabatic corrections to the scattering formalism for the description of electron stimulated desorption developed previously are investigated. It turns out that the cross-section for the desorption of ions derived earlier in the Born-Oppenheimer approximation remains essentially unaffected by these corrections (nonadiabatic effects being taken into account with sufficient accuracy in terms of the imaginary part of the BO potential for the ions). The cross-section for the desorption of reneutralized ions, however, which vanishes in BOA becomes nonzero. In semiclassical approximation the expression for the cross-section agrees with the result proposed earlier by Menzel and Gomer. The connection of the formalism with the Landau-Zener theory of nonadiabatic transitions is briefly discussed.
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Makoto Okusawa, Kouichi Ichikawa, Toshiyuki Matsumoto, Kenjiro Tsutsum ...
1982 Volume 51 Issue 6 Pages
1921-1926
Published: June 15, 1982
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The boron
K emission and absorption spectra of LaB
6, SmB
6 and EUB
6 have been measured to investigate the electronic band structure of the valence and conduction bands. For LaB
6 the observed emission spectrum is compared with the photoelectron spectrum and also with the energy-band calculations by means of a self-consistent augmented-plane-wave method. The result suggests that the B
K emission and absorption spectra are not influenced significantly by the presence of the localized 4
f electrons of the rare-earth ion and provide information on the electronic band structure of rare-earth hexaborides.
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Shoichi Annaka
1982 Volume 51 Issue 6 Pages
1927-1931
Published: June 15, 1982
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Interference phenomena between the σ and π components of linearly polarized X-rays are studied in the Laue case dynamical diffraction. It is shown experimentally that the polarization characteristics of the diffracted X-rays from Si change clearly with thicknesses of the specimen and elliptically polarized X-rays are produced by phase differences between the σ and π components. Theoretical calculations also confirm the experimental results.
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Yoshitada Murata
1982 Volume 51 Issue 6 Pages
1932-1935
Published: June 15, 1982
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A theoretical consideration in the formation of Kikuchi line concerning vibrational excitation is carried out from the double-scattering model of the Born approximation. The incident electrons excite a vibrational mode with an atomic displacement parallel to the incident wave vector. This result can be applied to estimate the magnitude of the surface rumpling.
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Kiyoshi Ueda, Yasuo Ashizawa, Kuniya Fukuda
1982 Volume 51 Issue 6 Pages
1936-1940
Published: June 15, 1982
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Relative oscillator strengths for about 30 transitions from the metastable 5
s5
p 3P levels of neutral strontium have been determined by using the hook method. The metastable levels are populated by the DC discharge. The oscillator strengths are placed on an absolute scale by reference to a recent lifetime measurement and relative intensity measurements. Our results are in reasonable agreement with other experimental and theoretical values.
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Kiyoshi Ueda, Masayoshi Karasawa, Kuniya Fukuda
1982 Volume 51 Issue 6 Pages
1941-1947
Published: June 15, 1982
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The 4
s4
p 3P levels of Zn have been populated by a DC discharge and three series of measurements have been applied to observe the 4
s4
p 3P-4
p2 3P multiplet at about λ2100 A. These are (1) precise measurement of the absorption profile for the
3P1-
3P2 autoionizing transition, (2) total-absorption measurement for the same transition with simultaneous dispersion (hook) measurement for the 4
s4
p 3P1-4
s5
s 3S1 transition at λ4722 A, and (3) simultaneous hook measurements for the
3P-
3P multiplet concerned and the 4
s4
p 3P-4
s5
s 3S visible multiplet. The autoionization rate of the 4
p2 3P2 level is 4.72×10
12 s
−1 from (1). From (2) and (3) the gf values are 0.76, 0.68, 0.68 and 0.97 for
3P1-
3P2,
3P0-
3P1,
3P1-
3P0 and
3P2-
3P1, respectively, by reference to the absolute
f values (∼0.14) for the visible multiplet.
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Kiyoshi Ueda, Yoshihiro Hamaguchi, Kuniya Fukuda
1982 Volume 51 Issue 6 Pages
1948-1952
Published: June 15, 1982
Released on J-STAGE: June 01, 2007
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We have measured Ar- and Kr-induced broadening of the Ca 4
s2 1S-4
snp 1P (6
≤n≤10) and 4
s2 1S-3
d4
p 1P transitions by means of the total absorption method. In this regime of
n, the broadening cross section increases to its maximum value with
n and then decreases. The maximum value is 28×10
−14 cm
2 at
n=8 for Ar and 72×10
−14 cm
2 at
n=9 for Kr. Assuming that the interatomic potential is described as a superposition of the Fermi potential and the polarization potential, we have calculated the cross section on the basis of the classical broadening theory. This calculation agrees well with both the present result and that for the Na 3
S-
nS transitions measured by Kachru
et al. by means of the trilevel-echo technique.
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Eiko Hiroike
1982 Volume 51 Issue 6 Pages
1953-1957
Published: June 15, 1982
Released on J-STAGE: June 01, 2007
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The indirect dephasing model for a vibrating molecule in a dense medium is succesively investigated by using the formulas obtained in the previous paper by the author. The line-shape function for the spectrum of the high-frequency mode is obtained, and the dependence of the line-width of the spectrum on the life-time of the excited state of the low-frequency mode is discussed.
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Kazuya Uehara, Takumi Yamamoto, Tsuneyuki Fujii, Norio Suzuki, Tsuyosh ...
1982 Volume 51 Issue 6 Pages
1958-1964
Published: June 15, 1982
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Boundary plasma of a circular tokamak has been investigated by means of electrostatic probes during lower-hybrid heating. The reflection coefficient is affected by the density gradient in front of the Iauncher. An effective ion heating is performed in the main plasma region when the boundary electron temperature is relatively high enough to suppress the parametric decay instabilities. The simultaneous injection of neutral beams as well as the lower-hybrid wave brings the suppression of instabilities with increase of the electron temperature coming from the neutral beam heating.
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Kanemitsu Katoh
1982 Volume 51 Issue 6 Pages
1965-1968
Published: June 15, 1982
Released on J-STAGE: June 01, 2007
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A formalism for the parametric instability with low-frequency magnetic field generation in a collisional plasma is developed. The spontaneous low-frequency magnetic field results from a resonant decay instability of an intense pump wave into a magneto-static wave which appears only in a collisional plasma. The growth rate for a resonant decay instability of an intense electromagnetic wave into a Langmuir wave and a magneto-static wave is obtained.
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Masahiro Wakatani, Tetsuji Abe
1982 Volume 51 Issue 6 Pages
1969-1974
Published: June 15, 1982
Released on J-STAGE: May 29, 2007
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Multi-helicity tearing modes are studied by use of reduced MHD equations based on a stellarator expansion. The
l=2 stellarator field has a tendency to limit magnetic braiding due to non-linear coupling between
m=2⁄
n=1 and
m=3⁄
n=2 tearing mode. For small external rotational transform of (
Remark: Graphics omitted.), however, disruption may occur for current profiles susceptible of it in a tokamak.
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Masayoshi Taguchi
1982 Volume 51 Issue 6 Pages
1975-1982
Published: June 15, 1982
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A simple expression of the fast-ion-induced current in the toroidal magnetic field is obtained by use of the adjoint drift-kinetic equation for electrons. The inverse aspect ratio is assumed to be small. The lowest-order terms of this ratio are retained in the calculation. By this expression, the beam-induced current for any beam distribution is easily evaluated. When the fast ions are monoenergetic, the beam-induced current is practically computed.
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Akira Yoshizawa
1982 Volume 51 Issue 6 Pages
1983-1991
Published: June 15, 1982
Released on J-STAGE: June 01, 2007
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The transport equation for energy dissipation rate in turbulent shear flows is examined by the use of a statistical theory, which is founded on the Direct-Interaction formalism as well as on the separation between the space and time scales of the mean and fluctuating fields. Various quantities appearing in the equation are expressed in terms of the turbulent energy and the energy dissipation rate as well as the mean velocity. On this basis, discussion is made on a model equation for energy dissipation rate which is frequently used in the turbulence closure models. As a result it is suggested that the usual model equation is not always justifiable from the standpoint of a statistical shear-turbulence theory.
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Koichi Tanaka, Shinya Ishii
1982 Volume 51 Issue 6 Pages
1992-1999
Published: June 15, 1982
Released on J-STAGE: June 01, 2007
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Scattering of a plane wave by a flow field induced by a vortex pair in translational motion is considered. The analysis of the scattered wave is facilitated by first order equations with respect to the wave component together with the Born approximation and by applying the Green’s function method. The directional distribution of the scattered wave and the total scattering cross section of the vortex pair are evaluated. Further, temporal variation of the scattered acoustic pressure,when the vortices pass by an observer fixed in space, is also plotted.
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Kaoru Fujimura
1982 Volume 51 Issue 6 Pages
2000-2009
Published: June 15, 1982
Released on J-STAGE: June 01, 2007
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The linear stability of Jeffery-Hamel inflow profiles is investigated on the basis of quasi-parallel theory. It is found that the critical Reynolds number
Rc increases monotonically as the shear stress at the wall τ
w increases and even a very small angle between the walls of a channel has a remarkable stabilizing effect. The critical phase velocity
cc reaches an asymptotic value of 0.1844 as τ
w→∞. Comparison of neutral stability curves from the Jeffery-Hamel flow and the two dimensional inlet flow is also discussed. Two kinds of approximations are made to asymptotic viscous solutions of the Orr-Sommerfeld equation, and the stability characteristics based on these approximations are compared with an exact solution obtained by using the step-by-step integrating procedure.
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G. Mandal, K. K. Mandal, G. Choudhury
1982 Volume 51 Issue 6 Pages
2010-2015
Published: June 15, 1982
Released on J-STAGE: June 01, 2007
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The effects of Hall current on Couette flow and heat transfer of a conducting fluid between two plates in a rotating system are discussed. Both Hall and rotation parameters introduce secondary velocity and secondary induced magnetic field. The resultant shear stress and heat transfer from the moving plate has been calculated assuming it to be non-conducting and taking the fixed plate to be infinitely conducting. The resultant shear stress increases with increase in Hartmann number as well as rotation parameter while it decreases with increase in Hall parameter. The role of each parameter on heat transfer is always opposite to its role on shear stress. In the absence of Hall current this opposing character remains unalterned even if direction of rotation is reversed.
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Mitsuhiro Tanaka
1982 Volume 51 Issue 6 Pages
2016-2023
Published: June 15, 1982
Released on J-STAGE: June 01, 2007
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Nonlinear self-modulation of waves propagating along the interface between two homogeneous liquid layers is investigated by means of the derivative expansion method. The stability characteristics of a uniform wavetrain are examined on the basis of the nonlinear Schrödinger equation. It is shown that the existence of the upper layer suppresses the modulational instability. Some limiting cases are discussed in connection with the Korteweg-de Vries equation and the Benjamin-Ono equation.
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C. Shen, V. C. Liu
1982 Volume 51 Issue 6 Pages
2024-2028
Published: June 15, 1982
Released on J-STAGE: June 01, 2007
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The stationary two-dimensional (
x,
z) near wakes behind a flat-based projectile which moves at a constant mesothermal speed (
V∞) along a
z-axis in a rarefied, fully ionized, plasma is studied using the wave model previously proposed by one of the authors (VCL). One-fluid theory is used to depict the free expansion of ambient plasma into the vacuum produced behind a fast-moving projectile. This nonstationary, one-dimensional (
x,
t) flow which is approximated by the K-dV equation can be transformed, through substitution,
t=
z⁄
V∞, into a stationary two-dimensional (
x,
z) near wake flow seen by an observer moving with the body velocity (
V∞). The initial value problem of the K-dV equation in (
x,
t) variables is solved by a specially devised numerical method. Comparisons of the present numerical solution for the asymptotically small and large times with available analytical solutions are made and found in satisfactory agreements.
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Miki Wadati, Kenji Ohkuma
1982 Volume 51 Issue 6 Pages
2029-2035
Published: June 15, 1982
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New types of solutions of completely integrable nonlinear evolution equations are found using the inverse scattering method. For the Modified Korteweg-de Vries equation the multiple-pole solutions, i.e., the solutions which correspond to multiple-pole of the reflection coefficient are investigated. Double-pole soltuion and triple-pole solution are obtained explicitly. It is shown that those solutions describe a weak-bound state of solitons and antisolitons.
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