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Proceedings of the International Symposium on Frontiers of Collective Motions (CM2002) : Aizu, Japan, 6-9 November 2002 /

The physics of nuclear collective motion was pioneered by A Bohr and B R Mottelson 50 years ago. Since then, experimental and theoretical development in this field has been remarkable under the leadership of the Copenhagen group. In the 21st century, a new era has opened up due to the recent develop...

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Detalles Bibliográficos
Clasificación:Libro Electrónico
Autor Corporativo: International Symposium on Frontiers of Collective Motions Aizu, Japan
Otros Autores: Sagawa, Hiroyuki, Iwasaki, Hironori
Formato: Electrónico Congresos, conferencias eBook
Idioma:Inglés
Publicado: [River Edge], N.J. : World Scientific, [2003]
Temas:
Acceso en línea:Texto completo

MARC

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111 2 |a International Symposium on Frontiers of Collective Motions  |d (2002 :  |c Aizu, Japan) 
245 1 0 |a Proceedings of the International Symposium on Frontiers of Collective Motions (CM2002) :  |b Aizu, Japan, 6-9 November 2002 /  |c edited by Hiroyuki Sagawa, Hironori Iwasaki. 
246 3 |a Frontiers of Collective Motions (CM2002) 
246 3 |a CM2002 
260 |a [River Edge], N.J. :  |b World Scientific,  |c [2003] 
300 |a 1 online resource :  |b illustrations 
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504 |a Includes bibliographical references. 
588 0 |a Print version record. 
505 0 |a Photo; Preface; CONTENTS; Cold Confined Clouds of Atoms are "Artificial Nuclei" Ben R. Mottelson (Nordita); Extended abstract; Slow Rotation of a Superfluid Trapped Fermi Gas P. Schuck (Orsay); 1. Introduction; 2. Linear response to a slow rotation; 3. Discussion; 4. Summary and outlook; Acknowledgments; References; Structure Study with AMD H. Horiuchi (Kyoto); 1. Introduction; 2. Characteristic features of AMD; 3. Neutron-rich isotopes of Be and B; 4. Island of Inversion around N=20; 5. Excited bands with many-particle many-hole structure in 44Ti; References. 
505 8 |a Extraction of Precise Gamow-Teller Quenching Value Q, Landau-Migdal Parameter g'N and Pion Condensation H. Sakai (Tokyo/CNS)1. Introduction; 2. 90Zr(p, n) and (n, p) Reactions at Tp ~ 300 MeV; 3. Results and Analysis; 3.1. MDA; 3.2. IVSM; 3.3. B(GT); 3.4. Sp- and Sp+; 3.5. Extraction of Q; 3.6. Extraction of g'NA; 4. Critical Density of Pion Condensation in Neutron Star; 5. Summary; Acknowledgments; References; Excitation of Isospin and Spin-Isospin Modes in the + Direction M.N. Harakeh (Groningen); 1. Introduction; 2. GT+ matrix elements from the (d,2He) and (t,3He) reactions. 
505 8 |a 3. GT+ matrix elements and electron-capture rates to 58Co4. Conclusions and outlook; Acknowledgments; References; New Aspects of L = 0 Magnetic Transitions in fp-Shell and Medium-Heavy Nuclei Y. Fujita (Osaka); 1. Introduction; 2. Experiment; 2.1. (3He, t) experiment; 2.2. GT transition strengths from CE reactions; 3. Comparison of analogous transitions; 3.1. Identification of isospin T of GT states; 3.2. Comparison of Tz = +1 to 0 GT transitions; 4. GT transitions of astrophysics interest; 5. GT strengths in medium-heavy nuclei; Acknowledgments; References. 
505 8 |a Mean-Field Approach to Superdeformed High-Spin States in 40Ca and Neutron-Rich 50S Regions K. Matsuyanagi (Kyoto)1. Introduction; 2. 40Ca region; 3. 50S region; 4. Summary; References; Chiral Doublet Bands in Triaxial Nuclei D.B. Fossan (SVNY at Stony Brook); 1. Introduction; 2. A ~ 130 chiral island: zh11/2 vh11/2 configuration; 3. Chirality fingerprints; 4. 104Rh chirality, ga9/2 vh11/2 configuration; 5. Conclusions; References; Reflection Asymmetric Shell Model for Octupole Rotation Y.S. Chen (CIAE); 1. Introduction; 2. Brief description of the model; 3. Calculations for Ra isotopes. 
505 8 |a 4. Octupole SD bands5. Summary; References; Chirality as a Window into Triaxiality: Odd-Odd Cs Isotopes T. Koike (SUNY at Stony Brook); 1. Introduction; 2. Systematics of reduced transition probability ratios: B(M1)/B(E2) and B(M1)In/B(Ml)Out; 3. Selection rules for AI=1 M1 and AI =2 E2 transitions for chiral geometry; 4. Conclusion; References; Proton Emission from Odd-Even and Odd-Odd Deformed Drip-Line Nuclei E. Maglione (Padova); 1. Introduction; 2. Decay widths for deformed Odd-Z even-N emitters; 3. Decay from odd-Z odd-N nuclei. 
520 |a The physics of nuclear collective motion was pioneered by A Bohr and B R Mottelson 50 years ago. Since then, experimental and theoretical development in this field has been remarkable under the leadership of the Copenhagen group. In the 21st century, a new era has opened up due to the recent developments of experimental facilities, especially radioactive ion beams and large?-ray arrays. Interest in collective motions is now shared in the research of other quantum many-body systems - for example, microclusters and Bose-Einstein condensation. It is therefore timely and important to review the c. 
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650 0 |a Nuclear collective models  |v Congresses. 
650 6 |a Modèles collectifs (Physique nucléaire)  |v Congrès. 
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700 1 |a Sagawa, Hiroyuki. 
700 1 |a Iwasaki, Hironori. 
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