2006
DOI: 10.1088/0305-4470/39/41/s04
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From relativistic quantum fields to condensed matter and back again: updating the Gross–Neveu phase diagram

Abstract: Abstract. During the last few years, the phase diagram of the large N Gross-Neveu model in 1+1 dimensions at finite temperature and chemical potential has undergone a major revision. Here we present a streamlined account of this development, collecting the most important results. Quasi-one-dimensional condensed matter systems like conducting polymers provide real physical systems which can be approximately described by the Gross-Neveu model and have played some role in establishing its phase structure. The kin… Show more

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Cited by 159 publications
(250 citation statements)
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“…(41) is limited to lower-dimensional modulations, the problem can be mapped onto a lower-dimensional one. In particular, the analytically known solutions of the 1 + 1 dimensional GN and NJL 2 models [51,52,53] can be utilized to construct solutions with one-dimensional modulations in 3 + 1 dimensions. The details of this very powerful method are discussed in the following.…”
Section: One-dimensional Modulationsmentioning
confidence: 99%
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“…(41) is limited to lower-dimensional modulations, the problem can be mapped onto a lower-dimensional one. In particular, the analytically known solutions of the 1 + 1 dimensional GN and NJL 2 models [51,52,53] can be utilized to construct solutions with one-dimensional modulations in 3 + 1 dimensions. The details of this very powerful method are discussed in the following.…”
Section: One-dimensional Modulationsmentioning
confidence: 99%
“…The lower part of Fig. 10 shows the quark number density for the solitonic solutions, which is proportional to [82,107,52,53] …”
Section: Solitonic Solutionsmentioning
confidence: 99%
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“…We choose the Gross-Neveu (GN) model in 1+1 dimensions [17] where in the large N limit all thermodynamic observables can easily be computed at both real and imaginary chemical potential, to any desired accuracy. Nevertheless the phase diagram at real µ is non-trivial, sharing qualitative properties with QCD (see [18] for a recent review). We then pretend that we are only able to compute all quantities at imaginary µ and try to extrapolate them to real µ, controlling our procedure against the exact results at each step.…”
Section: Introductionmentioning
confidence: 99%
“…More generally, the interaction of fermions with solitonic backgrounds could produce or affect a variety of interesting physical phenomena such as charge and fermion number fractionalization [79][80][81][82][83], hadron physics [68,69,[84][85][86], superfluidity [87,88], superconductivity [89], BoseEinstein condensation [90,91], conducting polymers [83,[92][93][94] and localization of fermions [95][96][97][98]. The spectrum of the fermion can in general be distorted due to the presence of such a background; bound states can appear and continuum states can change as compared with the free fermion.…”
Section: Introductionmentioning
confidence: 99%