Random matrix ensemble with random two-body interactions in the presence of a mean field for spin-one boson systems

For bosons carrying spin-one degree of freedom, we introduce an embedded Gaussian orthogonal ensemble of random matrices generated by random two-body interactions in the presence of a mean field that is spin (S) scalar [called BEGOE(1+2)-S1]. Embedding algebra for the ensemble, for m bosons in Ω num...

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Published inPhysical review. E, Statistical, nonlinear, and soft matter physics Vol. 88; no. 2; p. 022130
Main Authors Deota, H N, Chavda, N D, Kota, V K B, Potbhare, V, Vyas, Manan
Format Journal Article
LanguageEnglish
Published United States 01.08.2013
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Summary:For bosons carrying spin-one degree of freedom, we introduce an embedded Gaussian orthogonal ensemble of random matrices generated by random two-body interactions in the presence of a mean field that is spin (S) scalar [called BEGOE(1+2)-S1]. Embedding algebra for the ensemble, for m bosons in Ω number of single-particle levels (each triply degenerate), is U(3Ω)⊃G⊃G1⊗SO(3) with SO(3) generating the spin S. A method for constructing the ensemble for a given (Ω,m,S) has been developed. Numerical calculations show that (i) the form of the fixed-(m, S) density of states is close to a Gaussian; (ii) for a strong enough interaction, level fluctuations follow GOE; (iii) fluctuation in energy centroids is large; and (iv) spectral widths are nearly constant with respect to S for S<S(max)/2. Moreover, we identify two different pairing symmetry algebras in the space defined by BEGOE(1+2)-S1 and numerical results show that random interactions generate ground states with maximal value for the pair expectation value.
ISSN:1550-2376
DOI:10.1103/PhysRevE.88.022130