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Excitonic insulators and Gross-Neveu models

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arxiv 2112.07362 v1 pith:B7245IVW submitted 2021-12-14 cond-mat.str-el

classification cond-mat.str-el
keywords excitoniccriticaleqcpregimebehaviordifferentgross-neveuheat
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abstract

We introduce a generalized Gross-Neveu (GN) model to describe the excitonic instabilities in two different systems: a small overlap semi-metal (SM) and a small gap semi-conductor (SMC), both in two (2d) and three-dimensions (3d). We identify the excitonic order parameter (EOP) and obtain the effective potential within the Large $N$ limit approach where the GN model can be exactly solved. We obtain the excitonic insulator (EI) phase diagrams as a function of temperature, chemical potential, overlap between bands and gaps of the system. We show that the EI may undergo first- or second-order thermal transitions depending on the regime whereupon this phase is approached. We also investigate the expected thermodynamic signatures for the specific heat above the fine-tuned excitonic quantum critical point (EQCP), in both 2d and 3d, in the SMC regime. We show that the EQCP is a different kind of critical point since although the EOP vanishes at the EQCP, there is always a finite gap in the SMC regime. We find that for high temperatures, the specific heat might exhibit a scaling behavior in the form $C_V/T \propto T^{(d-z)/z}$, where $d$ is the dimension of the system and $z$ is the dynamical critical exponent. The very low temperature behavior has a dominant exponential thermally activated term due to the presence of a gap that does not vanish at the excitonic transition.

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Cited by 1 Pith paper

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. OpenAlex reports about 8 citations worldwide. Full citation record

  1. Generalized Beth-Uhlenbeck Approach to the 2+1D Gross-Neveu Model

    cond-mat.mes-hall 2026-04 conditional novelty 5.0 of 10

    Generalized Beth-Uhlenbeck entropy density suppresses low-energy Landau damping in the 2+1D Gross-Neveu model while preserving bound-state effects, yielding a sharper exciton-to-fermion Mott crossover.

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