Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Finite Temperature Phase Transitions in the multicomponent Hubbard model

昌久 古賀, Akihisa Koga

Published Jul 1, 2016• 0 citations
OpenAlex

Related papers

Finite-temperature phase transitions in the SU(N) Hubbard model

大将 梁取, Hiromasa Yanatori, 昌久 古賀 +1 more

•Jan 1, 2016•0 citations

Finite-temperature phase transitions in the SU(N) Hubbard model

Hiromasa Yanatori, Akihisa Koga

We investigate the $\mathrm{SU}(N)$ Hubbard model for the multicomponent fermionic optical lattice system, combining dynamical mean-field theory with the continuous-time quantum Monte Carlo method. We obtain the finite-temperature phase diagrams with $N\ensuremath{\le}6$ and find that low-temperature properties depend on the parity of the components. The magnetically ordered state competes with the correlated metallic state in the system with an even number of components $(N\ensuremath{\ge}4)$, yielding the first-order phase transition. It is also clarified that in the odd-component system, the ordered state is realized at relatively lower temperatures and the critical temperature is constant in the strong coupling limit.

arXiv:1603.02647•Physical review. B./Physical review. B•Jul 18, 2016•23 citations

Finite-temperature phase diagram of the Hubbard model

G. Migliorini, A. Nihat Berker

arXiv:cond-mat/9811233•The European Physical Journal B•Aug 1, 2000•4 citations

Dicke model for a multicomponent system

Igor K. Kudryavtsev, A N Meleshko, A. S. Shumovskiǐ

A study is made of a phase transition in a multicomponent system of two-level atoms interacting with a finite set of electromagnetic field modes. It is shown that the coupling between the components increases the temperature of a phase transition to a state characterized by ordering in the atomic subsystem and simultaneous filling of the photon modes.

Soviet Journal of Quantum Electronics•Nov 30, 1979•1 citation

Phase transition in two-dimensional multicomponent Bose liquid: a new type of quasi-long-range order

I. V. Tokatly

The $ν$-component two-dimensional (2D) Bose liquid is considered. It is shown that the finite temperature phase transition exists in this 2D continuously degenerate multicomponent system. The new type of quasi-long-range order occurs as a result of this transition. The correlation function in ordered state is a product of the power-law XY-universality class type function and the exponential function corresponding to the $SU(ν)$ invariant model. The transition temperature is calculated for the diluted system. It is found that the physical mechanism of the phase transition is changed when $ν$ exceeds the critical value $ν_c = 4$. The experimental realization of the considered model is discussed briefly.

arXiv:cond-mat/9801130•Jan 14, 1998•0 citations

Quantum Phase transitions in Hubbard lattices

Matteo Rizzi, Rosario Fazio

•Jan 1, 2007•1 citation
We investigate the SU(N)\mathrm{SU}(N)SU(N) Hubbard model for the multicomponent fermionic optical lattice system, combining dynamical mean-field theory with the continuous-time quantum Monte Carlo method. We obtain the finite-temperature phase diagrams with $N\ensuremath{\le}6$ and find that low-temperature properties depend on the parity of the components. The magnetically ordered state competes with the correlated metallic state in the system with an even number of components $(N\ensuremath{\ge}4)$, yielding the first-order phase transition. It is also clarified that in the odd-component system, the ordered state is realized at relatively lower temperatures and the critical temperature is constant in the strong coupling limit.
The ννν-component two-dimensional (2D) Bose liquid is considered. It is shown that the finite temperature phase transition exists in this 2D continuously degenerate multicomponent system. The new type of quasi-long-range order occurs as a result of this transition. The correlation function in ordered state is a product of the power-law XY-universality class type function and the exponential function corresponding to the SU(ν)SU(ν)SU(ν) invariant model. The transition temperature is calculated for the diluted system. It is found that the physical mechanism of the phase transition is changed when ννν exceeds the critical value νc=4ν_c = 4νc​=4. The experimental realization of the considered model is discussed briefly.