Embedded GOE Ensembles for Interacting Boson Systems: BEGOE(1+2) for Spinless Bosons

Author(s):  
V. K. B. Kota
Keyword(s):  
2009 ◽  
pp. 375-387
Author(s):  
Sascha Zllner ◽  
Hans-Dieter Meyer ◽  
Peter Schmelcher
Keyword(s):  

2004 ◽  
Vol 45 (8) ◽  
pp. 3086-3094 ◽  
Author(s):  
Richard L. Hall ◽  
Wolfgang Lucha ◽  
Franz F. Schöberl

1961 ◽  
Vol 123 (2) ◽  
pp. 699-705 ◽  
Author(s):  
Fumihiko Takano

1993 ◽  
Vol 223 (5) ◽  
pp. 277-308 ◽  
Author(s):  
Hong-Wei He ◽  
Roger Alan Smith
Keyword(s):  

2004 ◽  
Vol 243 (1-6) ◽  
pp. 131-143 ◽  
Author(s):  
J. Dukelsky ◽  
G.G. Dussel ◽  
S. Pittel

Entropy ◽  
2018 ◽  
Vol 20 (7) ◽  
pp. 541 ◽  
Author(s):  
Venkata Kota ◽  
Narendra Chavda

Embedded ensembles or random matrix ensembles generated by k-body interactions acting in many-particle spaces are now well established to be paradigmatic models for many-body chaos and thermalization in isolated finite quantum (fermion or boson) systems. In this article, briefly discussed are (i) various embedded ensembles with Lie algebraic symmetries for fermion and boson systems and their extensions (for Majorana fermions, with point group symmetries etc.); (ii) results generated by these ensembles for various aspects of chaos, thermalization and statistical relaxation, including the role of q-hermite polynomials in k-body ensembles; and (iii) analyses of numerical and experimental data for level fluctuations for trapped boson systems and results for statistical relaxation and decoherence in these systems with close relations to results from embedded ensembles.


Author(s):  
KARL-HEINZ FICHTNER ◽  
LARS FICHTNER ◽  
KEI INOUE ◽  
MASANORI OHYA
Keyword(s):  

2018 ◽  
Vol 60 (11) ◽  
pp. 2105
Author(s):  
Е.В. Васинович ◽  
А.С. Москвин ◽  
Ю.Д. Панов

Abstract —A 2D anisotropic system of S = 1 centers of the charge triplet type in systems with variable valence or “semi-hard-core” boson systems with a limitation for the occupation of lattice sites n = 0, 1, 2 is studied in the framework of the pseudospin formalism. Assuming that the ground state is a quantum paramagnet, the pseudo-spin wave spectrum and also the conditions of the condensation of pseudomagnons with a phase transition to a superconducting state have been found using the Schwinger boson method.


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