{"arxiv_id":"hep-ph/0406159","incoming":{"papers":32,"sentences":60,"groups":[{"kind":"extends","label":"Builds on it","papers":1,"sentences":1,"quotes":[{"arxiv_id":"2009.13363","title":"Non-Hermitian BCS-BEC crossover of Dirac fermions","url":"/paper/2009.13363","section":"Conclusions and outlook","sentence":"A partial list is given below. * To incorporate the competition between the chiral condensate and the diquark condensate (i.e., a competition between a Dirac mass and a Majorana mass) along the lines of [ref] * To investigate collective fluctuations around the saddle points and test the validity of the mean-field approximation for non-Hermitian * To analytically prove numerical findings in this work, e.g., the existence of a nontrivial solution to the gap equation for large $g$ * To examine dissipative under an external magnetic field that catalyzes [ref] * To study $(1)_A$ vortices * To study the effect of nonzero $μ$ on non-Hermitian * To analyze the structure of Cooper pairs as a function of the complex coupling, and provide a more precise description of the non-Hermitian BCS-BEC crossover * To use the renormalization group to improve the mean-field analysis * To clarify how to apply ","intent_p":0.81,"contests_p":null}]},{"kind":"method_or_tool","label":"Uses its method or tool","papers":1,"sentences":1,"quotes":[{"arxiv_id":"0705.0792","title":"Larkin-Ovchinnikov-Fulde-Ferrell state in two-color quark matter","url":"/paper/0705.0792","section":"INTRODUCTION","sentence":"We will make use of a mean-field model to address this issue by following a line of argument of Ref. [ref] , which looks successful in reproducing the numerical results of lattice two-color QCD [ref] .","intent_p":0.9,"contests_p":null}]},{"kind":"comparison","label":"Compares with it","papers":7,"sentences":10,"quotes":[{"arxiv_id":"1112.5401","title":"Quark-meson-diquark model for two-color QCD","url":"/paper/1112.5401","section":"Diquark condensation","sentence":"The resulting chemical potential dependence of the chiral and diquark condensates at zero temperature is shown in Fig. [ref] where we compare the prediction from leading order chiral perturbation theory [ref] , the NJL [ref] and the linear sigma model [ref] results with lattice data [ref] and our quark-meson-diquark model mean-field result with vacuum contribution from Eqs. ([ref]), ([ref]).","intent_p":1.0,"contests_p":null},{"arxiv_id":"2211.01789","title":"Probing the hadron mass spectrum in dense two-color QCD with the linear sigma model","url":"/paper/2211.01789","section":"Linear sigma model","sentence":"The critical chemical potential ([ref]) is the same as the result from chiral perturbation theory [ref] and NJL model [ref] , and suggested numerically by lattice simulations [ref] .","intent_p":0.98,"contests_p":null},{"arxiv_id":"2312.17017","title":"Mass spectrum of spin-one hadrons in dense two-color QCD: Novel predictions by extended linear sigma model","url":"/paper/2312.17017","section":"Analytic derivation of $μ_q^cr = m_π^(H)/2$ in the eLSM","sentence":"In Sec. 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Pith's classifier typed each sentence. A label is shown at intent probability 0.8 or more (0.95 for support), a contest at 0.7 or more. Measured accuracy against two blind model families is at https://pith.science/accuracy. The quoted sentences are the citing authors' own.","held_up":null,"_links":{"html":"https://pith.science/paper/hep-ph/0406159"}}