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Theoretical and Mathematical Physics

Bose-Einstein condensation in the excited band and the energy spectrum of the Bose-Hubbard model

Ihor V. Stasyuk, O. V. Velychko

Published Sep 1, 2011• 4 citations
Publisher
DOI
10.1007/s11232-011-0110-2

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Phase transition into the phase with Bose-Einstein (BE) condensate in the two-band Bose-Hubbard model with the particle hopping in the excited band only is investigated.Instability connected with such a transition (which appears at excitation energies δ < |t ′ 0 |, where |t ′ 0 | is the particle hopping parameter) is considered.The re-entrant behaviour of spinodales is revealed in the hard-core boson limit in the region of positive values of chemical potential.It is found that the order of the phase transition undergoes a change in this case and becomes the first one; the re-entrant transition into the normal phase does not take place in reality.First order phase transitions also exist at negative values of δ (under the condition δ > δ crit ≈ -0.12|t ′ 0 |).At µ < 0 the phase transition mostly remains to be of the second order.The behaviour of the BE-condensate order parameter is analyzed, the (Θ, µ) and (|t ′ 0 |, µ) phase diagrams are built and localizations of tricritical points are established.The conditions are found at which the separation on the normal phase and the phase with the BE condensate takes place.

arXiv:1103.5662•Condensed Matter Physics•Jan 1, 2011•7 citations
We investigate the fermion spectrum within the Bose–Fermi–Hubbard model used for the description of boson-fermion mixtures of ultra-cold atoms in optical lattices. We used the method based on the Hubbard operator approach for an on-site basis. The equation for fermion Green’s function in the Bose–Fermi–Hubbard model is built; Green’s functions of higher orders are decoupled in the Hubbard-I approximation (the case of the strong on-site interaction). The corresponding spectral densities are calculated. In the case of hard-core bosons, the condition of appearance of additional bands in the fermion spectrum is investigated. It is shown that these bands exist only in the state with a Bose–Einstein condensate and appear because of the mixing of states with different numbers of bosons. These additional bands can be interpreted as a manifestation of composite excitations (when the appearance of a fermion on the site is accompanied by the simultaneous creation (or annihilation) of a boson).
The excitation spectrum of a spin-orbit coupled Bose-Einstein condensate is investigated by the use of the Bose-Hubbard model and a mean-field approach. The undiagonalized Hamiltonian matrix for a general inversion-symmetric Bravais lattice is found. Analytical expressions for the excitation spectrum is then found in the limiting case of on-site interactions and nearest-neighbor hopping on a one-dimensional chain and a two-dimensional quadratic lattice. The densities of particles in the ground state acting as mean-field parameters are found self-consistently by minimization of the free energy, and they are seen to be in agreement with published literature.
Phase transition into the phase with Bose-Einstein (BE) condensate in the two-band Bose-Hubbard model with the particle hopping in the excited band only is investigated.Instability connected with such a transition (which appears at excitation energies δ < |t ′ 0 |, where |t ′ 0 | is the particle hopping parameter) is considered.The re-entrant behaviour of spinodales is revealed in the hard-core boson limit in the region of positive values of chemical potential.It is found that the order of the phase transition undergoes a change in this case and becomes the first one; the re-entrant transition into the normal phase does not take place in reality.First order phase transitions also exist at negative values of δ (under the condition δ > δ crit ≈ -0.12|t ′ 0 |).At µ < 0 the phase transition mostly remains to be of the second order.The behaviour of the BE-condensate order parameter is analyzed, the (Θ, µ) and (|t ′ 0 |, µ) phase diagrams are built and localizations of tricritical points are established.The conditions are found at which the separation on the normal phase and the phase with the BE condensate takes place.