We study Bose-Einstein condensation (BEC) in three-dimensional two-component bosonic gases, character- izing the universal behaviors of the critical modes arising at the BEC transitions. For this purpose, we use field-theoretical (FT) renormalization-group (RG) methods and perform mean-field and numerical calculations. The FT RG analysis is based on the Landau-Ginzburg-Wilson ! 4 theory with two complex scalar fields which has the same symmetry as the bosonic system. In particular, for identical bosons with exchange Z2 symmetry, coupled by effective density-density interactions, the global symmetry is Z2,e ⊗ U(1) ⊗ U(1). At the BEC transition, it may break into Z2 ,e ⊗ Z2 ⊗ Z2 when both components condense simultaneously, or to U(1) ⊗ Z2 when only one component condenses. This implies different universality classes for the corresponding critical behaviors. Numerical simulations of the two-component Bose-Hubbard model in the hard-core limit support the RG prediction: when both components condense simultaneously, the critical behavior is controlled by a decoupled XY fixed point, with unusual slowly decaying scaling corrections arising from the onsite interspecies interaction.
Bose-Einstein condensation and critical behavior of two-component bosonic gases / Ceccarelli, Giacomo; Nespolo, Jacopo; Pelissetto, Andrea; Vicari, Ettore. - In: PHYSICAL REVIEW A. - ISSN 1050-2947. - STAMPA. - 92:4(2015), p. 043613. [10.1103/PhysRevA.92.043613]
Bose-Einstein condensation and critical behavior of two-component bosonic gases
PELISSETTO, Andrea;
2015
Abstract
We study Bose-Einstein condensation (BEC) in three-dimensional two-component bosonic gases, character- izing the universal behaviors of the critical modes arising at the BEC transitions. For this purpose, we use field-theoretical (FT) renormalization-group (RG) methods and perform mean-field and numerical calculations. The FT RG analysis is based on the Landau-Ginzburg-Wilson ! 4 theory with two complex scalar fields which has the same symmetry as the bosonic system. In particular, for identical bosons with exchange Z2 symmetry, coupled by effective density-density interactions, the global symmetry is Z2,e ⊗ U(1) ⊗ U(1). At the BEC transition, it may break into Z2 ,e ⊗ Z2 ⊗ Z2 when both components condense simultaneously, or to U(1) ⊗ Z2 when only one component condenses. This implies different universality classes for the corresponding critical behaviors. Numerical simulations of the two-component Bose-Hubbard model in the hard-core limit support the RG prediction: when both components condense simultaneously, the critical behavior is controlled by a decoupled XY fixed point, with unusual slowly decaying scaling corrections arising from the onsite interspecies interaction.File | Dimensione | Formato | |
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