-
Masayoshi Tajiri, Youichi Murakami
1989 Volume 58 Issue 9 Pages
3029-3032
Published: September 15, 1989
Released on J-STAGE: June 01, 2007
JOURNAL
RESTRICTED ACCESS
N-periodic soliton solutions that consist of
N sequences of the algebraic localized solitons in arbitrary directions are presented to the Kadomtsev-Petviashvili equation with positive dispersion using the bilinear transformation method. The existence conditions and some properties of them are also given.
View full abstract
-
Takehiko Oguchi, Hidetsugu Kitatani
1989 Volume 58 Issue 9 Pages
3033-3036
Published: September 15, 1989
Released on J-STAGE: June 01, 2007
JOURNAL
RESTRICTED ACCESS
The specific heats at the critical temperatures of the dual lattice of the Ising model on a square lattice were calculated by the canonical series of cluster approximations. Then the specific heats of the original lattice were calculated through the dual transformation. Finally the critical exponent α′ below the transition temperature was determined as α′=0 by the coherent-anomaly method.
View full abstract
-
Shigeru Odaka, Takahiko Kondo, Koya Abe, Katsuya Amako, Yasuo Arai, Yu ...
1989 Volume 58 Issue 9 Pages
3037-3041
Published: September 15, 1989
Released on J-STAGE: June 01, 2007
JOURNAL
RESTRICTED ACCESS
A possible contribution of neutral scalar bosons to the cross section of multihadron production at
e+e− collisions was examined at center-of-mass energies between 55.0 and 60.8 GeV by taking into account first-order radiative corrections. We found no positive evidence and established new upper limits on the coupling parameter of the scalars.
View full abstract
-
Keiji Matsuo, Yukinari Homan, Katsunori Muraoka, Masanori Akazaki, Shi ...
1989 Volume 58 Issue 9 Pages
3042-3045
Published: September 15, 1989
Released on J-STAGE: May 29, 2007
JOURNAL
RESTRICTED ACCESS
Electron density fluctuations in Heliotron E were measured using the Fraunhofer-diffraction method of a CO
2 laser radiation. The deduced dispersion relation was found to be consistent with the drift wave, Doppler-shifted by a poloidal rotation resulting from a radial electric field. The measured intensities of the fluctuations were used to estimate the diffusion coefficient and particle confinement time, the latter (10 ms) being the same order of magnitude as that obtained independently from laser fluorescence and plasma emission, both at the Balmer alpha line.
View full abstract
-
Masaru Aniya, Hideo Okazaki, Michisuke Kobayashi
1989 Volume 58 Issue 9 Pages
3046-3048
Published: September 15, 1989
Released on J-STAGE: May 29, 2007
JOURNAL
RESTRICTED ACCESS
A new approach to interpret the origin of the ultrasonic attenuation in superionic conductors is proposed. On the basis of experimental evidence such as the structural analysis and the molecular dynamics results, it is suggested that the sound attenuation due to mobile ions can be evaluated through the formalism of the liquid theory.
View full abstract
-
Shuji Ogata, Setsuo Ichimaru
1989 Volume 58 Issue 9 Pages
3049-3052
Published: September 15, 1989
Released on J-STAGE: June 01, 2007
JOURNAL
RESTRICTED ACCESS
We report the first microscopic observation by Monte Carlo simulation (
N=1458) of how the particle correlations and bond-orientational orders develop in supercooled one-component plasmas at the freezing transitions. It is found that a formation of particle layers expedites a subsequent evolution into a metastable state and that the final states have bcc-crystalline layered structures with an admixture of a few intralayer interstitials.
View full abstract
-
Yoshihiro Yamada, Yasukage Oda, Naoki Kawaji, Hideki Yamagata, Kunisuk ...
1989 Volume 58 Issue 9 Pages
3053-3056
Published: September 15, 1989
Released on J-STAGE: May 29, 2007
JOURNAL
RESTRICTED ACCESS
The dc magnetic susceptibility of YBa
2(Cu
1−xM
x)
3O
y with M=Fe and Co (
x<0.08) annealed in high-pressure oxygen gas was measured in the normal state. The annealing was done in flowing oxygen gas of about 6 kg/cm
2 for 24 hours at low temperatures (350–450°C) after an ordinary annealing in air. Although the O
2 annealing markedly enhances the superconducting transition temperature, the measured susceptibilities of Fe and Co substituents were essentially unchanged. The dc magnetic susceptibilities of the air- and O
2-annealed samples with Ni (
x<0.08) were also measured and found to be the same. In this compound, the Ni atom was found to have a magnetic moment close to that of the Ni
2+ ion (
S=1,
Peff=2.83 μ
B).
View full abstract
-
Kazuyoshi Yoshimura, Takashi Imai, Tadashi Shimizu, Yutaka Ueda, Koji ...
1989 Volume 58 Issue 9 Pages
3057-3060
Published: September 15, 1989
Released on J-STAGE: May 29, 2007
JOURNAL
RESTRICTED ACCESS
Nuclear magnetic/quadrupole resonance (NMR/NQR) has been observed for the Cu nuclei in La
2−xSr
xCuO
4. NMR measurements have been carried out for the powdered sample whose
c axes are aligned. No evidence for magnetic ordering was observed down to 1.3 K. Instead, the existence of two sets of
63⁄65Cu resonances due to nonequivalent Cu sites has been concluded from the results of spectrum and relaxation measurements at low temperatures. These resonances are ascribed to the effect of the charge differentiation introduced by the substitution of Sr for La.
View full abstract
-
Takashi Sakuma, Kaoru Shibata
1989 Volume 58 Issue 9 Pages
3061-3064
Published: September 15, 1989
Released on J-STAGE: June 01, 2007
JOURNAL
RESTRICTED ACCESS
Neutron inelastic scattering of solid electrolyte β-Cu
2Se was measured by the time-of-flight (TOF) method at room temperature. Low-lying dispersionless excitations near hω∼3.4 meV, which would be common to copper ion conductors, existed in the β-phase. This result was compared with those of the excitations in other solid electrolytes.
View full abstract
-
Akira Onuki
1989 Volume 58 Issue 9 Pages
3065-3068
Published: September 15, 1989
Released on J-STAGE: June 01, 2007
JOURNAL
RESTRICTED ACCESS
We introduce a Ginzburg-Landau model for solid solutions to examine elastic effects near the phase separation. As a first application the spinodal curve is calculated when the elastic moduli depend on the concentration and an external stress is applied. The instability is triggered by fluctuations with wave vectors in particular directions. This indicates the morphology of emerging domains.
View full abstract
-
Akira Onuki
1989 Volume 58 Issue 9 Pages
3069-3072
Published: September 15, 1989
Released on J-STAGE: June 01, 2007
JOURNAL
RESTRICTED ACCESS
We calculate an effective free energy for a concentration field by eliminating elastic fields which are coherently induced by concentration inhomogeneities. We obtain long-range interactions for solids generally under external stress when the elastic moduli weakly depend on
c. They radically influence the domain morphology in late stages of the phase separation process.
View full abstract
-
Tatsuoki Takeda, Tomonori Takizuka
1989 Volume 58 Issue 9 Pages
3073-3076
Published: September 15, 1989
Released on J-STAGE: June 01, 2007
JOURNAL
RESTRICTED ACCESS
With respect to cold fusion, a fractofusion mechanism is investigated. Deuterons are accelerated by the electric field generated between crack surfaces in a crystal. By assuming the possible magnitude of the potential difference, we calculate the fusion rate and energy multiplication factor. The results are consistent with those of the cold fusion experiments, and the fractofusion mechanism can explain the cold fusion phenomena successfully.
View full abstract
-
Michiaki Matsukawa, Shinsuke Watanabe, Hiroshi Tanaca
1989 Volume 58 Issue 9 Pages
3077-3080
Published: September 15, 1989
Released on J-STAGE: May 29, 2007
JOURNAL
RESTRICTED ACCESS
A two-dimensional generalization of the higher order approximation in the reductive perturbation method is investigated. The fluid equations for plasma are adopted as the model equations in the two-dimensional space. It is found that the technique of renormalization is applicable to the two-dimensional system such as the fluid equations for plasma.
View full abstract
-
Michiaki Matsukawa, Shinsuke Watanabe, Hiroshi Tanaca
1989 Volume 58 Issue 9 Pages
3081-3084
Published: September 15, 1989
Released on J-STAGE: June 01, 2007
JOURNAL
RESTRICTED ACCESS
The higher order approximation for the two-dimensional nonlinear LC circuit equation is studied by the Hirota method. It is found that the Hirota method is effective not only for the completely integrable and weakly perturbed systems but also for the higher order approximation.
View full abstract
-
Hidenori Takahashi, Kimiaki Konno
1989 Volume 58 Issue 9 Pages
3085-3088
Published: September 15, 1989
Released on J-STAGE: June 01, 2007
JOURNAL
RESTRICTED ACCESS
We consider initial value problems for the modified Korteweg-de Vries equation by using the inverse scattering method. We find that simple initial potentials produce a double pole and breather solutions as well as soliton solutions. We observe a soliton which connects distantly two isolated potentials.
View full abstract
-
Nobuhiko Saitô, Yasushi Matsunaga
1989 Volume 58 Issue 9 Pages
3089-3105
Published: September 15, 1989
Released on J-STAGE: June 01, 2007
JOURNAL
RESTRICTED ACCESS
Inadequacy of perturbation treatment in chaotic dynamics is pointed out, especially for phase space distribution function. The coarse graining is introduced into phase space distribution function for describing macroscopic thermodynamic process as a necessary and inevitable procedure for the transition from microscopic to macroscopic levels. A concept of convergence in law is employed for coarse graining. Thus a new approach to the linear response theory is presented, which can remove the various difficulties in the conventional linear response theory. The derivation of the distribution function in the sense of convergence in law is left open, but it is expected that the principal results such as fluctuation-dissipation theorem, Kubo formula for kinetic coefficient remain valid, provided that an appropriate interpretation is applied. Furthermore the entropy is shown to increase and the susceptibility derived in this theory is adiabatic susceptibility expected as a thermodynamic process. The present formulation will provide an answer to the critical discussion by van Kampen.
View full abstract
-
Tsuyoshi Horiguchi
1989 Volume 58 Issue 9 Pages
3106-3110
Published: September 15, 1989
Released on J-STAGE: June 01, 2007
JOURNAL
RESTRICTED ACCESS
We propose an exactly soluble Ising model with two kinds of exchange integrals on a square lattice. We assume that the number of bonds on which the exchange integrals take a value is even around each elementary plaquette; we name such a plaquette an even-bonds plaquette. We find two phase transition temperatures in the Ising model. We have a magnetic phase transition at one of them and a phase transition relating to the ordering of a dual spins introduced by a dual transformation of bond variables at the other. The latter phase transition is investigated in detail and turned out to have a relation with the confinement of odd-bonds plaquettes in a generalized system. Both phase transitions are of Onsager type.
View full abstract
-
Junji Suzuki
1989 Volume 58 Issue 9 Pages
3111-3122
Published: September 15, 1989
Released on J-STAGE: June 01, 2007
JOURNAL
RESTRICTED ACCESS
Some thermodynamic quantities in the
N state vertex model (the SAA model) are obtained. It is shown that the surface tension and the correlation length are the same as those of the six-vertex model. The mean square height difference 〈
h2〉 between the central site and perimeter sites is also calculated. It turns out that the usual fluctuation theory does not give the correct relation between 〈
h2〉 and the correlation length.
View full abstract
-
Naoki Kawashima, Masuo Suzuki
1989 Volume 58 Issue 9 Pages
3123-3130
Published: September 15, 1989
Released on J-STAGE: June 01, 2007
JOURNAL
RESTRICTED ACCESS
The super-effective-field theory (SEFT) proposed by one of the present authors (M.S.) is applied to the antiferromagnetic planar model on a two-dimensional triangular lattice (AFPT model) in order to understand the nature of chiral order by a series of mean-field-type approximations. Approximants are constructed for clusters of various sizes up to 651 sites and calculated by use of the Monte Carlo technique. The critical temperature
Tc and the exponent γ are estimated as
Tc=0.5096(5) and γ=1.7(2) respectively. Some of characteristic features of this model such as the relation between the KT-like and Ising-like transitions are discussed from a viewpoint of the present theory.
View full abstract
-
Tôru Sakai, Minoru Takahashi
1989 Volume 58 Issue 9 Pages
3131-3142
Published: September 15, 1989
Released on J-STAGE: June 01, 2007
JOURNAL
RESTRICTED ACCESS
We investigate the Heisenberg antiferromagnets on the square lattice with different coupling constants in two directions of bonds such that the ratio is
J(=
J⊥⁄
J⁄⁄). For
S=1⁄2 and
S=1, we estimate the critical value
Jc such that Néel order exists for
Jc<
J≤1, while not for 0≤
J<
Jc. The results of the spin wave theory suggest that
Jc is very small (
Jc<10
−1) and a disordered phase exists only in quasi-one-dimensional regions. Then we treat interchain couplings as a mean field. By this approximation
Jc is derived from
Jc=(2χ
st)
−1 where χ
st is the staggered susceptibility of a chain. We estimate χ
st for finite chains by the exact diagonalization of the hamiltonian and extrapolate to infinite systems. Our estimations are
Jc=0 for
S=1⁄2 and
Jc≥0.025 for
S=1.
View full abstract
-
Hideki Iimura, Takeshi Seo, Shigeru Yamada
1989 Volume 58 Issue 9 Pages
3143-3150
Published: September 15, 1989
Released on J-STAGE: May 29, 2007
JOURNAL
RESTRICTED ACCESS
Gamma-gamma angular correlations on 20 cascades in the decay of 12 min
151Nd have been measured. The spins of levels at 426.4, 507.9, 524.3, 532.0, 840.9 and 1133.1 keV in
151Pm have been uniquely determined to be 1/2, 5/2, 3/2, 7/2, 3/2 and 5/2, respectively. The E2/M1 mixing ratios of 6 transitions have been derived. The obtained results have been discussed on the basis of the rotation-vibration coupling model.
View full abstract
-
Ichiro Yamada, Atsunori Danjo, Takato Hirayama, Atsushi Matsumoto, Shu ...
1989 Volume 58 Issue 9 Pages
3151-3156
Published: September 15, 1989
Released on J-STAGE: May 29, 2007
JOURNAL
RESTRICTED ACCESS
The crossed ion-and-electron-beams technique has been used to measure the absolute cross sections for single ionization of F
+, Ne
+, Cl
+ and Ar
+ ions by electron impact, over the electron energy range from below threshold up to 1000 eV. For F
+ and Cl
+ ions, the present experiment has provided the first absolute ionization cross sections. The measured cross sections for F
+ and Ne
+ ions are well reproduced with the semiempirical Lotz formula over the energy range investigated. The results for Cl
+ and Ar
+ ions show more rapid rise from the threshold than the prediction of the Lotz formula, indicating the contribution of excitation-autoionization processes, and tend to be in good agreement with the Lotz formula at higher energies.
View full abstract
-
Yuji Nakamura, Katsuji Ichiguchi, Masahiro Wakatani, John L. Johnson
1989 Volume 58 Issue 9 Pages
3157-3174
Published: September 15, 1989
Released on J-STAGE: June 01, 2007
JOURNAL
RESTRICTED ACCESS
Two-dimensional MHD equilibrium and stability codes based on the stellarator expansion provide a good description of the properties of three-dimensional stellarator configurations. Improvements and extensions of the two-dimensional stellarator expansion of such codes with a particular emphasis on the STEP code are discussed. Three-dimensional equilibria of the ATF Torsatron at zero and finite beta are given. The relation between the Mercier stability criterion and low-
n stability limit with respect to pressure driven modes is clarified, where
n is a toroidal mode number. Whenever
DI\gtrsim0.2, the STEP code predicts global unstable modes numerically, where
DI is the Mercier parameter whose shear stabilization term is normalized as −1⁄4. The second stability regime is realized by controlling the magnetic axis position by the vertical field in an
l=2 and
M=12 torsatron/heliotron configuration, where
l is a pole number and
M is a helical period number of the magnetic field.
View full abstract
-
Hironobu Kasano, Hiroyuki Mashiyama
1989 Volume 58 Issue 9 Pages
3175-3181
Published: September 15, 1989
Released on J-STAGE: June 01, 2007
JOURNAL
RESTRICTED ACCESS
The crystal structure of [N(CH
3)
4]
2NiCl
4 was investigated at 23°C in phase I (normal phase), at −5°C in phase III (commensurate phase) and at −60°C in phase IV (normal phase) by means of X-ray diffraction. The least-squares calculations converged at
R=0.043 for phase I, at
R=0.047 for phase III and at
R=0.036 for phase IV, respectively. It was revealed that each tetrahedral ion is in disorder in phase I. In phase III, the position of each molecule almost coincides with one of two disordered sites in phase I. It was confirmed in phase IV that the rotating direction of each molecule about the axis parallel to the
b-axis is in-phase and the rotation angle of NiCl
42− tetrahedron is about two times larger than that in phase I.
View full abstract
-
Yasuo Saruyama
1989 Volume 58 Issue 9 Pages
3182-3197
Published: September 15, 1989
Released on J-STAGE: June 01, 2007
JOURNAL
RESTRICTED ACCESS
Minimum potential structure composed of helical polymer molecules is studied. The intramolecular potential and the intermolecular potential between the nearest neighbor molecules are taken into account. Attending to the geometric symmetry of the system general features of the minimum potential structure is investigated. The process to build up the bulk structure from a couple of molecules which are of the minimum potential packing is given in detail. Unperiodic structures as well as periodic structures are found to be the minimum potential structures. Crystallographic space groups of the periodic structures are given. Some periodic structures belong to lower symmetry systems than their lattices.
View full abstract
-
Yukio Shibata, Kimihiro Ishi, Toshiaki Ohsaka
1989 Volume 58 Issue 9 Pages
3198-3203
Published: September 15, 1989
Released on J-STAGE: June 01, 2007
JOURNAL
RESTRICTED ACCESS
The lattice dynamics of molecular crystal CS
2 is studied within the rigid molecule and harmonic approximations, on the basis of Kihara core potential. Frequencies of lattice vibrations, dispersion curves, density of states and heat capacity at low temperatures are calculated. The results are in good agreement with experimental data and also compared with previous calculations. A role of nonaxisymmetric short-range interactions is discussed.
View full abstract
-
Yoshie Matsuo, Kaori Miyata
1989 Volume 58 Issue 9 Pages
3204-3211
Published: September 15, 1989
Released on J-STAGE: June 01, 2007
JOURNAL
RESTRICTED ACCESS
X-ray diffuse scattering measurements have been carried out on β-phase Au-47.5 at%Cd-0.75 at%Cu and Au-49.0 at%Cd-0.75 at%Cu alloys. Five notable features were found in the distribution of diffuse scattering: (i) diffuse sheets extending uniformly parallel to the (111) planes, (ii) diffuse streaks running through the fundamental reflection points in the [1\bar10] directions, (iii) diffuse peaks near
q=(1⁄3)[110] along the [1\bar10] direction, (iv) diffuse peaks near
q=(1⁄3)[112] along the [11\bar2] direction and (v) diffuse peaks near
q=(3⁄4)[110] along the [110] direction. The intensity of these five kinds of anomalous diffuse scattering shows characteristic temperature dependence. The diffuse scattering is discussed in relation to the mechanism of martensitic transformation.
View full abstract
-
Norimichi Kojyo, Yositaka Onodera
1989 Volume 58 Issue 9 Pages
3212-3218
Published: September 15, 1989
Released on J-STAGE: June 01, 2007
JOURNAL
RESTRICTED ACCESS
To understand the role of hydrogens in the ferroelectricity of hydrogen-bonded crystals, the effect of deuteration in the mixed crystal Cs(H
1−xD
x)
2PO
4 is studied on the basis of the coupled proton-dipole model presented by the present authors (J. Phys. Soc. Jpn.
57 (1988) 4391) for pure CsH
2PO
4 and CsD
2PO
4. The model is essentially reduced to a one-dimensional Ising system with random bonds, and the static dielectric constant is analytically obtained in the paraelectric phase. Variation of the ferroelectric phase transition temperature with deuteration,
TC(
x), is calculated. The result predicts that the
TC(
x) curve of Cs(H
1−xD
x)
2PO
4, which has not yet been determined by experiments, should have a large bowing because of the quasi-one-dimensionality of the system.
View full abstract
-
Ryuzo Abe, Tomonari Dotera
1989 Volume 58 Issue 9 Pages
3219-3226
Published: September 15, 1989
Released on J-STAGE: June 01, 2007
JOURNAL
RESTRICTED ACCESS
High temperature expansion for ln
Z (
Z: the partition function in the absence of magnetic field) of the Ising model on the Penrose lattice is discussed. The terms up to the order of
w8 are derived. To illustrate an extrapolation procedure employed here, the critical compressibility factor
Zc and the correlation function
C at
Tc for the neighboring spin pair are first treated in the case of two-dimensional square lattice. It turns out that the terms up to
w8 for ln
Z lead to the results within the error of 0.2∼0.3% as compared to exact values. Along the same line,
Zc and \bar
C (average correlation function) are calculated for the Penrose lattice. The final results are
Zc=0.138±0.002 and \bar
C=0.673±0.003.
View full abstract
-
Yositaka Onodera, Norimichi Kojyo
1989 Volume 58 Issue 9 Pages
3227-3235
Published: September 15, 1989
Released on J-STAGE: June 01, 2007
JOURNAL
RESTRICTED ACCESS
Motivated by Tokunaga’s proposal that ratio of the paraelectric dipole moment μ
c to the saturation dipole moment μ
s is correlated with whether a ferroelectric substance belongs to the displacive or order-disorder type, we calculated the two dipole moments for the classical coupled an harmonic-oscillator model in the independent-site approximation. It is found that μ
c⁄μ
s\gtrapprox1 in the displacive type and μ
c⁄μ
s≈1 in the order-disorder type. Thus, the ratio indeed has some correlation with the types of ferroelectric phase transitions, but its magnitude alone is insufficient in discriminating the two types. In addition, our theory predicts a certain relation between μ
c⁄μ
s and the discontinuity of the specific heal at
Tc, which BaTiO
3 is shown to satisfy strikingly well.
View full abstract
-
Riki Kawashima
1989 Volume 58 Issue 9 Pages
3236-3242
Published: September 15, 1989
Released on J-STAGE: June 01, 2007
JOURNAL
RESTRICTED ACCESS
The AC conductivities have been measured in the frequency range from 3 Hz to 100 kHz at temperatures in the phases II and I along the
b-axis of CsNO
3 crystal to study the dynamical properties near the structural phase transition point
Ttr. The frequency dependence of conductivities varies at
Ttr. The spectra of conductivities on the complex conductivity plane show polydispersive relaxation processes in both the phases. The conductivities for the
b-axis of the crystal have been compared with those for the
c-axis. The effective relaxation time τ(
T) can be evaluated from the experimental results and described by activation type in phase I. The behavior of τ(
T) shows a stepwise change near
Ttr.
View full abstract
-
Tomio Iwasaki, Toshio Soda
1989 Volume 58 Issue 9 Pages
3243-3250
Published: September 15, 1989
Released on J-STAGE: June 01, 2007
JOURNAL
RESTRICTED ACCESS
We develop the Green function theory for the high-field phase of the bcc solid
3He. We adopt decoupling procedures, which do not contradict the spin wave theory at temperatures near
T=0. The magnetization is determined by solving two self-consistent equations and we obtain the
H-
T phase diagram. According to our results, the bcc
3He has only one first-order transition above the low-field phase.
View full abstract
-
Ryoichi Suzuki, Makoto Osawa, Shoichiro Tanigawa, Makoto Matsumoto, No ...
1989 Volume 58 Issue 9 Pages
3251-3263
Published: September 15, 1989
Released on J-STAGE: June 01, 2007
JOURNAL
RESTRICTED ACCESS
The three dimensional electron-positron momentum densities have been obtained on Ti and Zr from measurements of two dimensional angular correlation of positron annihilation radiation followed by an image reconstruction technique based on direct Fourier transformation. Augmented-plane wave band structure calculations have been carried out and the results are compared with the experiments. Agreement between the experiment and the theory leads to a conclusion that both Ti and Zr have electron surface sheets which are centered at H and hole surface sheets which are running along the
Γ-A axis.
View full abstract
-
Yoshihiro Asai
1989 Volume 58 Issue 9 Pages
3264-3269
Published: September 15, 1989
Released on J-STAGE: June 01, 2007
JOURNAL
RESTRICTED ACCESS
Carrier locations of hole-doped and electron-doped high-
Tc copper oxides in their ground states were determined by quantum chemical calculations. We have used a cluster surrounded by point charges. The used point charge arrangement produces a potential which simulates the functional form of the Madelung potential completely. Our calculation includes electronic correlations especially of on-site Coulomb repulsion of the Cu atom, which is the most important near the half-filling of the ground state. The doped hole will occupy the oxygen 2p
π band. The doped electron will occupy the Cu 4s band. In the hole-doped and the electron-doped copper oxide, a moment on the Cu
3dx2−y2 orbital will remain.
View full abstract
-
Nobuhiko Sakai, Nobuhiro Shiotani, Fumitake Itoh, Ou Mao, Masahisa Ito ...
1989 Volume 58 Issue 9 Pages
3270-3279
Published: September 15, 1989
Released on J-STAGE: June 01, 2007
JOURNAL
RESTRICTED ACCESS
Compton profiles of silicon along the [100] and [110] axes have been measured with a recently developed spectrometer having a momentum resolution of 0.084 atomic units. The following subjects are discussed using the observed profiles: (1) valence electron profiles, (2) directional anisotropy of the profile, (3) comparison with the angular correlation of positron-annihilation radiation, (4) evaluation of the Lock-Crisp-West theory, and (5) the auto correlation function. The high resolution in momentum makes it possible to evaluate theoretical calculations precisely. It is shown that the theoretical calculation based on the tight binding model describes the momentum distribution of silicon fairly well.
View full abstract
-
Naoshi Suzuki, Takahiro Yamasaki, Kazuko Motizuki
1989 Volume 58 Issue 9 Pages
3280-3289
Published: September 15, 1989
Released on J-STAGE: June 01, 2007
JOURNAL
RESTRICTED ACCESS
Systematic APW band calculations are carried out for the non-magnetic states of intercalation compounds M
1⁄3, TiS
2 (M=Mn, Fe, Co, Ni), and differences and similarities of the electronic band structures for different intercalant M atoms are clarified. The results obtained explain various physical properties observed for M
1⁄3TiS
2. Calculations of the bond orders are also carried out in order to elucidate the bonding nature of M atoms in the intercalation compounds.
View full abstract
-
Nobuhisa Fujima, Tsuyoshi Yamaguchi
1989 Volume 58 Issue 9 Pages
3290-3297
Published: September 15, 1989
Released on J-STAGE: May 29, 2007
JOURNAL
RESTRICTED ACCESS
Magnetism and electronic structure of Ni
N clusters are calculated by the spin-polarized DV–Xα–LCAO method for
N=4, 6, 8, 13, 14 and 19. The valence 3
d electrons are localized within the atoms of the clusters and separated from the 4
s valence electrons which extend over the whole cluster. The 4
s electronic states well correspond to those of the shell model. Since the highest occupied molecular orbital is within the 3
d band, there exist 3
d holes. Physically, the number is 2 for 4<
N<8, 8 for 8≤
N≤18, and 18 for
N=19 and 20. This results in the stepwise change of magnitude of the total spin as a function of
N. This 3
d magnetic anomaly is closely related to the 4
s shell structure and expected to appear in a series of transition-metal clusters. This anomaly is different from the so-called Kubo effect of fine particles of simple metals.
View full abstract
-
Susumu Misawa
1989 Volume 58 Issue 9 Pages
3298-3303
Published: September 15, 1989
Released on J-STAGE: June 01, 2007
JOURNAL
RESTRICTED ACCESS
The Hubbard model is examined in the strong correlation limit within the framework of the Hubbard-I-type simple-decoupling method of the Green’s functions. The decouplings are made with the projection operators. The transition temperature
Tc of the
s- and
d-wave superconductivity due to the superexchange interaction is calculated as a function of the hole concentration δ. The resultant
Tc becomes zero as δ→0 and δ→1, and can have appreciable values in some regions of δ. The
d-wave superconductivity is favorable when δ∼1⁄3, while
s-wave state is favorable in other regions.
View full abstract
-
Kenji Yonemitsu, Yasushi Wada
1989 Volume 58 Issue 9 Pages
3304-3323
Published: September 15, 1989
Released on J-STAGE: June 01, 2007
JOURNAL
RESTRICTED ACCESS
The effect of anisotropy is studied for superconductivity due to electron-phonon coupling. Parameters in the model are so determined that they can reproduce the results of band calculations and the phonon dispersion relations of La
2−xSr
xCuO
4. The electron-phonon coupling strength and the dopant concentration are varied over a wide range. We first calculate the phonon polarization part and then solve numerically the Eliashberg-Nambu equation which includes anisotropies of Fermi surface, the phonons, and the coupling. It turns out that the electron-phonon coupling is less anisotropic than the electronic density of states, even when the Fermi surface is close to the van Hove singularity. The superconducting transition temperature is predominantly determined by the averaged electron-phonon coupling over the Fermi surface. As carrier concentration changes and the Fermi surface crosses the configuration with the van Hove singularity, the transition temperature is expected to have a cusp.
View full abstract
-
Hiroyuki Oyanagi, Yoshikazu Nishihara, Keizo Murata, Hirotaka Yamaguch ...
1989 Volume 58 Issue 9 Pages
3324-3327
Published: September 15, 1989
Released on J-STAGE: May 29, 2007
JOURNAL
RESTRICTED ACCESS
The effect of hole doping on the electron states at the copper sites in La
2−xSr
xCuO
4−y (0.0<
x<0.25) has been studied by the X-ray absorption near-edge structure on the Cu K-edge. We find that the absorption edge shifts to a higher energy with the increase of Sr concentration
x and saturates at
x=0.20, coinciding with
x having the maximum value of
Tc. The observed systematic edge shift indicates that
doping influences the electron states on the copper sites either directly, by the formation of the Cu d hole (d
8 configuration) or indirectly, through the distortion of the CuO
6 unit.
View full abstract
-
Shunya Abe, Hiromi Nakazawa, Takejiro Kaneko, Hajime Yoshida, Kazuo Ka ...
1989 Volume 58 Issue 9 Pages
3328-3333
Published: September 15, 1989
Released on J-STAGE: June 01, 2007
JOURNAL
RESTRICTED ACCESS
Measurements on the magnetic properties of the intermetallic compounds RCu
4Pd (R=Gd, Tb, Dy, Ho and Er) with a cubic crystal structure are carried out in the temperature range from 4.2 to 300 K under magnetic fields up to 150 kOe. All the compounds are found to be ferromagnetic. Temperature variations of the susceptibilities follow the Curie-Weiss law in higher temperature. The paramagnetic Curie temperature for each compound is in good agreement with the Curie temperature. The effective magnetic moment per R ion coincides well with that derived from the free R
3+ ion. The results are discussed in terms of the RKKY theory.
View full abstract
-
Tosizumi Aoki
1989 Volume 58 Issue 9 Pages
3334-3338
Published: September 15, 1989
Released on J-STAGE: June 01, 2007
JOURNAL
RESTRICTED ACCESS
From the point of view of the quantum lattice liquid, an attempt is made to understand the one-dimensional
S=1⁄2 Heisenberg antiferromagnet. Without assuming a long-range order, the spin wave excitation is approximately derived from the motion of a number operator (
z-component spin). With the aid of a sum rule, the spectrum is estimated. The Boson representation of the system is approximately given on the basis of the equation of motion of the number operator. In this framework, the susceptibility, the specific heat and the correlation function are calculated. The results imply the possibility of a quantum lattice liquid description of the system.
View full abstract
-
Yoshitami Ajiro, Hiroki Yamazaki, Kenji Kawaguchi, Nobuyoshi Hosoito, ...
1989 Volume 58 Issue 9 Pages
3339-3346
Published: September 15, 1989
Released on J-STAGE: June 01, 2007
JOURNAL
RESTRICTED ACCESS
Ferromagnetic resonance (FMR) of multilayered metallic films synthesized from an insoluble combination of Fe and Mg is studied in a temperature range from 10 K to 300 K. A well defined FMR signal is observed in each sample with Fe thickness ranging from 4 Å to 30 Å. The observed spectra are found to be strongly dependent on the regularity of the layered structure. The resonance field exhibits an unusual shift which changes systematically as a function of the thickness as well as temperature. The origin of the shift of the resonance field is discussed in relation to the amorphous-like structure observed for the thickness less than 12 Å.
View full abstract
-
Atsunobu Nakamura, Norio Kawakami, Ayao Okiji
1989 Volume 58 Issue 9 Pages
3347-3354
Published: September 15, 1989
Released on J-STAGE: June 01, 2007
JOURNAL
RESTRICTED ACCESS
The ultrasonic attenuation coefficient and the elastic constant are investigated for the heavy-fermion system UPt
3. The effects of the antiferromagnetic spin fluctuation are taken into consideration by means of the hydrodynamic theory. It is shown that the spin thermal fluctuation gives rise to the peak structure for the attenuation coefficient near the temperature characteristic of the antiferromagnetic spin fluctuation. Furthermore, it is expected that the elastic constant has a dip structure in the same temperature regime due to the same origin. The above results are qualitatively in agreement with the experimental findings for UPt
3.
View full abstract
-
Fumihiro Matsukura, Y\={u}ichi Tazuke, Tomonao Miyadai
1989 Volume 58 Issue 9 Pages
3355-3360
Published: September 15, 1989
Released on J-STAGE: June 01, 2007
JOURNAL
RESTRICTED ACCESS
For Ising spin glasses Fe
xTiS
2 (
x=0.05, 0.1, 0.2), to investigate the temperature dependence of the relaxation time, ac-susceptibility measurements are made. Frequency dependences of spin glass transition temperatures defined by the maximum of the ac-susceptibility are analyzed by four conventional equations. The appropriate equation for
x=0.05 and
x=0.1 is the power law (for finite
T*). For
x=0.1 it seems that the Fulcher law also describes the data. The appropriate equation for
x=0.2 is the Fulcher law. The results of the analyses suggest the existence of clusters of Fe-spins for high-Fe concentrations.
View full abstract
-
Kazuyoshi Takeda, Hiroyuki Deguchi, Takahiro Hoshiko, Kensuke Konishi, ...
1989 Volume 58 Issue 9 Pages
3361-3370
Published: September 15, 1989
Released on J-STAGE: May 29, 2007
JOURNAL
RESTRICTED ACCESS
Magnetic and thermal properties have been studied on two kinds of organic free radicals, TANOL(2,2,6,6-tetramethyl-4-piperidinol-1-oxyl) and TPV(1,3,5-triphenylverdazyl), where the unpaired electrons are localized on the NO bond in the former compound but delocalized on the larger molecular orbitals in the latter. TANOL has been confirmed magnetically as a typical one-dimensional Heisenberg system with localized quantum spins coupled with the exchange constant
J⁄
kB=−5.2 K. On the other hand, the experimental results on TPV can not reasonably be understood on the basis of a localized model with the possible paths of magnetic interactions such as a railroad trestle lattice. It is suggested that organic free radicals offer promising real systems for getting essential physical phenomena which can check model Hamiltonians for a delocalized and frustrated quantum system.
View full abstract
-
Mihoko Yoshida, Kazuo Morigaki
1989 Volume 58 Issue 9 Pages
3371-3382
Published: September 15, 1989
Released on J-STAGE: May 29, 2007
JOURNAL
RESTRICTED ACCESS
Triplet exciton states in a-Si:H, a-Si,C:H and a-Si,N:H were investigated by the steady-state and time-resolved optically detected magnetic resonance techniques. The existence of triplet exciton states in a-Si:H and a-Si,N:H materials was confirmed, for the first time from these measurements. The extent of the electron orbitals in the triplet exciton state and its averaged lifetime in these materials were estimated to be ∼10 A and ∼1 ms, respectively. A singlet-triplet exciton splitting energy in a-Si:H was also estimated to be ∼0.15 eV. An impurity-related center and a self-trapped exciton center are considered as the origin for the triplet exciton centers in these materials.
View full abstract
-
Hidehiko Wakabayashi, Tsuneaki Goto, Kazuaki Fukamichi, Hiroyuki Komat ...
1989 Volume 58 Issue 9 Pages
3383-3391
Published: September 15, 1989
Released on J-STAGE: May 29, 2007
JOURNAL
RESTRICTED ACCESS
Mössbauer spectra have been measured for two Fe-rich amorphous alloys,
a-Fe
91.5La
8.5 with spin glass behavior and
a-Fe
82.5La
17.5 with reentrant spin glass behavior, in the temperature range between 4.2 K and room temperature. These spectra are analyzed using the Hesse and Rubertsch method to obtain the distribution of hyperfine fields. The distribution of hyperfine fields at 4.2 K consists of a main component ranging from 200 kOe to 400 kOe and a sub-component around 150 kOe. The average Fe-moment is estimated to be 1.96μ
B for
a-Fe
91.5La
8.5 and 2.00μ
B for
a-Fe
82.5La
17.5. Hyperfine fields in
a-Fe
91.5La
8.5 appear progressively below 150 K, which is apparently higher than the spin glass temperature of 124 K determined by the ac susceptibility measurement. On the other hand, hyperfine fields in
a-Fe
82.5La
17.5 appear just below the ferromagnetic ordering temperature of 267.5 K, but increase anomalously below 70 K. This anomaly can be explained in terms of the freezing of transverse components of spins.
View full abstract
-
M. A. Gaffar, G. F. Al-Noaimi, A. Abu El-Fadl
1989 Volume 58 Issue 9 Pages
3392-3400
Published: September 15, 1989
Released on J-STAGE: May 29, 2007
JOURNAL
RESTRICTED ACCESS
Dielectric permittivity, ε
22, spontaneous polarization,
Ps, and coercive field,
Ec, of triglycine sulphate (TGS) crystals doped with d-l alanine, orthonitroaniline, paranitroaniline or aniline molecules have been measured from room temperature up to the transition point. A remarkable displacement of the hysteresis loops of polarization along the direction of the field axis and a broadened transition from the polar to the non-polar phase are detected. An increase in the value of
Ps and a decrease of both ε
22 and
Ec are also observed. The changes in both ε
22 and
Ps attributed to the creation by the dopants of an internal electric field,
Eb. The internal bias affects the Curie constant and ε
max in a way similar to that introduced by an external bias. The value of
Eb in the vicinity of the phase transition and the parameters of the statistical dipolar theory of ferroelectricity have been calculated.
View full abstract
-
Haruhiko Suzuki, Fuminao Shimizu, Toshihisa Yamaguchi, Masaaki Takashi ...
1989 Volume 58 Issue 9 Pages
3401-3405
Published: September 15, 1989
Released on J-STAGE: June 01, 2007
JOURNAL
RESTRICTED ACCESS
Single crystals of ferroelectric K
2CoCl
4 have been obtained by the Bridgman method and the dielectric, thermal and dilatometric properties have been investigated. The phase-transition sequence of this crystal was confirmed to be analogous to that of other Rb
2ZnCl
4-group ferroelectrics.
View full abstract