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Article type: Cover
1980 Volume 61 Issue 2 Pages
Cover1-
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Article type: Appendix
1980 Volume 61 Issue 2 Pages
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Article type: Appendix
1980 Volume 61 Issue 2 Pages
249-250
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[in Japanese]
Article type: Article
1980 Volume 61 Issue 2 Pages
251-
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Article type: Article
1980 Volume 61 Issue 2 Pages
252-257
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Article type: Article
1980 Volume 61 Issue 2 Pages
258-267
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Article type: Article
1980 Volume 61 Issue 2 Pages
268-270
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Article type: Article
1980 Volume 61 Issue 2 Pages
270-273
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Article type: Article
1980 Volume 61 Issue 2 Pages
273-283
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Article type: Article
1980 Volume 61 Issue 2 Pages
283-287
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Article type: Article
1980 Volume 61 Issue 2 Pages
287-292
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Article type: Article
1980 Volume 61 Issue 2 Pages
293-295
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Article type: Article
1980 Volume 61 Issue 2 Pages
295-298
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Article type: Article
1980 Volume 61 Issue 2 Pages
298-300
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Article type: Article
1980 Volume 61 Issue 2 Pages
300-301
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Article type: Article
1980 Volume 61 Issue 2 Pages
301-307
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Article type: Article
1980 Volume 61 Issue 2 Pages
307-311
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Article type: Appendix
1980 Volume 61 Issue 2 Pages
313-
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1980 Volume 61 Issue 2 Pages
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Article type: Article
1980 Volume 61 Issue 2 Pages
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1980 Volume 61 Issue 2 Pages
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1980 Volume 61 Issue 2 Pages
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Article type: Article
1980 Volume 61 Issue 2 Pages
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1980 Volume 61 Issue 2 Pages
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1980 Volume 61 Issue 2 Pages
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Article type: Article
1980 Volume 61 Issue 2 Pages
317-
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Article type: Article
1980 Volume 61 Issue 2 Pages
317-318
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1980 Volume 61 Issue 2 Pages
318-
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Article type: Article
1980 Volume 61 Issue 2 Pages
318-
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Article type: Appendix
1980 Volume 61 Issue 2 Pages
319-320
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Article type: Article
1980 Volume 61 Issue 2 Pages
321-329
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Macroscopic structure of giant resonance states is explored with use of semi-classical models based on the model-independent sum rules.
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Article type: Article
1980 Volume 61 Issue 2 Pages
329-333
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1980 Volume 61 Issue 2 Pages
334-340
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An expression of the RPA-energy weighted sum rule for spin-dependent multipole operators is derived and used to relate the sum rule value to the Fermi liquid parameters, including the effect of the tensor force. Numerical results for the 'exchange' contribution to the sum rule are presented and discussed. It is shown that the M2 strength recently observed from the electron scattering experiment exhausts only about 20% of the energy weighted sum rule value.
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1980 Volume 61 Issue 2 Pages
340-345
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1980 Volume 61 Issue 2 Pages
345-353
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(1) Electroexcitations of electric giant multipole resonances (GR) of strongly deformed nuclei (^<238>U, ^<152>Sm, ^<24>Mg) were studied systematically. ^<238>U, ^<152>Sm... 0^+GR (breathing mode) was not affected by nuclear deformation and was seen between two 1^-GR (K^π0^-, 1^-) peaks. 2^+GR (K^π=0^+, 1^+, 2^+) spectrum was reproduced with small splitting (≅2 MeV). ^<24>Mg... Measured spectrums were unfolded into multipole distributions (C1,..,C6). C1 component was very similar to (γ, n) spectrum. C2, C3 components were widely distributed up to E_X≅34 MeV. 6^+ state (1d_<5/2>^<-1>, -1g_<9/2>) was discovered at 9.92 MeV. (2) Backward inelastic electron scattering from ^<90>Zr (θ=155°) and ^<24>Mg(θ=180°) were measured to study their transverse excitations. ^<90>Zr... Spin dependent E1, M2 GR's are expected between E_X=11 and 25 MeV. ^<24>Mg... 2nd peak of M1 form factor of the 10.65 MeV, T=1, 1^+ state was measured. Strong enhancement was observed as compared to (1d_<5/2>^<-1>, 1d_<3/2>) form factor.
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Article type: Article
1980 Volume 61 Issue 2 Pages
353-362
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General nuclear rotations including precession and wobbling motions are studied by both time -dependent variational method and "double variational method". Shortcomings and advantages of the cranking model and the angular momentum projection method are investigated. A method which removes the shortcoming and takes over the advantages is suggested.
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Article type: Article
1980 Volume 61 Issue 2 Pages
363-368
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The model of i_<13/2> particles coupled to a soft rotor, which is described using the angular momentum projection method applied to coherent boson states, is applied to the Er isotopes using the full shell model space for i_<13/2>. The properties of the wave functions of g-band and S-band are discussed.
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Article type: Article
1980 Volume 61 Issue 2 Pages
368-376
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The cranked Hartree-Fock-Bogoliubov theory is extended by introducing each different angular frequency with respect to intruder and core motions. The quasi-stable solutions for band crossing region are found by the present approach for ^<158>Er. The wave functions can not be connected between two bands.
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Y. Tanaka, R. Okamoto, S. Suekane
Article type: Article
1980 Volume 61 Issue 2 Pages
376-381
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Hamamoto's remedy for the band crossing anomalies is investigated using a schematic model. It is shown that the remedy is applicable only in the vicinity of the band crossing point. The main point of her prescription is to diagonalize the particle-rotor model Hamiltonian which includes the inter-band interaction h, using the basis constructed from the solutions of the cranking model by excluding h which is the origin of the anomalies. Consequently, the resulting wave functions show the anomalously sharp and large peak in the angular momentum fluctuation in the band crossing region. The matrix element of h results in the state-dependent gap parameter under the Marshalek's a priori assumption on the pairing interaction in the rotating frame.
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A. Iwamoto
Article type: Article
1980 Volume 61 Issue 2 Pages
381-385
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Mass parameter at finite temperature is discussed starting from the cranking formula. A general discussion about the disappearance of the shell effect and about the relation to the liquid drop value is given. A special attention is given to the stretching motion for which we calculated the mass parameters related to the harmonic oscillator potential and to the Fermi gas. In both cases, the equivalence of the cranking mass and the incompressible irrotational liquid drop value is shown.
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Article type: Article
1980 Volume 61 Issue 2 Pages
386-389
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1980 Volume 61 Issue 2 Pages
390-392
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A simple model of collective modes in a nucleus "rotating" about the symmetry axis is derived on the basis of the cranked harmonic oscillator model. The two-body effective interaction is determined self-consistently by using the Landau theory of Fermi liquids. The RPA dispersion equation can be solved exactly. Obtained RPA modes are as follows. i) Collective modes corresponding to the usual giant quadrupole modes in a axially symmetric deformed nucleus. Each degenerate ± K component splits. (K=1, 2) ii) The collective rotational mode. From a classical point of view, this mode corresponds to the motion of a symmetric top moving freely. iii) The spurious mode, which can be normalized. iv) The non-collective mode in the neighborhood of the yrast line.
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Article type: Article
1980 Volume 61 Issue 2 Pages
392-395
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The side feeding times of γ-rays to yrast states emitted from highly excited high-spin states are discussed. Theoretical values are compared with experimental ones and the origins of the discrepancies between them are also discussed.
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T. Otsuka
Article type: Article
1980 Volume 61 Issue 2 Pages
395-406
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A review on the microscopic structure of the collective state in the transitional nuclei is presented. The favoured pair concept of Hecht et al. is first introduced. Various methods of collective state construction are investigated from the favoured pair point of view, and the importance of the seniority projection is emphasized. Effects of non S-D or non collective states are discussed, and it is suggested that the 4^+ collective pair plays a significant role. The truncation in the boson expansion technique is also discussed, and a serious problem is pointed out.
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Nobuaki Yoshida, Akito Arima
Article type: Article
1980 Volume 61 Issue 2 Pages
406-413
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The Ginocchio model is used to study the Intreacting Boson Approximation. In order to derive its boson Hamiltonian from the fermion Hamiltonian of the Ginocchio model, we use the Boson Expansion Technique with s- and d-bosons and the Otsuka-Arima-Iachello method. The results of calculation show that the Interacting Boson Model with the two Hamiltonians given by those two methods are good approximations to exact solutions. We also study the Boson Expansion with d-bosons only after the BCS transformation. The results show that this is not a good approximation.
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T. Otsuka
Article type: Article
1980 Volume 61 Issue 2 Pages
413-418
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Recent development of the microscopic foundation of the proton-neutron interacting boson model is presented. The boson Hamiltonian is constructed microscopically in a degenerate single particle orbit shell. The Hamiltonian contains effects of non S-D states through renormalization of relevant terms, but still consists of one- and two-body terms. Spectra obtained by this Hamiltonian can be compared well with those obtained in the shell model diagonalization.
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T. Kishimoto
Article type: Article
1980 Volume 61 Issue 2 Pages
418-428
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This report is essentially the review of what I have been doing in the past ten years in collaboration with Drs. T. Tamura and K. Weeks at the University of Texas at Austin, USA. However, instead of duplicating our published works, I would like to emphasize physical concepts we have kept in mind throughout our study.
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Y. Miyanishi, G. Watanuki
Article type: Article
1980 Volume 61 Issue 2 Pages
429-433
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It is shown that the pairing rotational mode can be expressed in terms of the special quasi-boson mode with zero energy (Goldstone boson mode) by introducing the intrinsic Hamiltonian free from pairing rotation under the RPA. The coupling between pairing rotation and intrinsic excitations is investigated as the interplay of this special eigenmode and the intrinsic modes due to the effects neglected in the RPA.
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[in Japanese]
Article type: Article
1980 Volume 61 Issue 2 Pages
434-
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Article type: Article
1980 Volume 61 Issue 2 Pages
434-439
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