2007
DOI: 10.1103/physrevd.75.096003
|View full text |Cite
|
Sign up to set email alerts
|

Relativistic BCS-BEC crossover at zero temperature

Abstract: We investigate the BCS-BEC crossover at zero temperature in the frame of a relativistic model. The universality of the BCS-BEC crossover for non-relativistic systems breaks down in relativistic case and the crossover can be induced by changing the density. When the effective scattering length is much less than the fermion Compton wavelength, we recover the non-relativistic result if the gas is initially in non-relativistic state. At ultra-strong coupling where the scattering length is of the order of the Compt… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

0
28
0

Year Published

2009
2009
2017
2017

Publication Types

Select...
6
1

Relationship

0
7

Authors

Journals

citations
Cited by 41 publications
(28 citation statements)
references
References 16 publications
0
28
0
Order By: Relevance
“…Going through the standard steps of converting the random matrix theory to a sigmamodel we find in the limit N → ∞ that g RMT ν (Ĵ) = g ν ( √ 2NĴ), which shows that the random-matrix partition function is equivalent to the finite-volume partition function, 45 provided that the dimensionless random-matrix diquark sources and singular values (i.e., the square roots of the eigenvalues of A T A) are related to the physical quantities bŷ…”
Section: Intermediate Densitymentioning
confidence: 93%
See 1 more Smart Citation
“…Going through the standard steps of converting the random matrix theory to a sigmamodel we find in the limit N → ∞ that g RMT ν (Ĵ) = g ν ( √ 2NĴ), which shows that the random-matrix partition function is equivalent to the finite-volume partition function, 45 provided that the dimensionless random-matrix diquark sources and singular values (i.e., the square roots of the eigenvalues of A T A) are related to the physical quantities bŷ…”
Section: Intermediate Densitymentioning
confidence: 93%
“…This phenomenon is called (relativistic) BEC-BCS crossover. It passes a number of nontrivial tests [21,22,26], and its possible realization in dense quark matter in QCD has been investigated in various model calculations [27][28][29][30][31][32][33][34][35][36][37][38][39][40][41][42] (see also [43][44][45][46][47][48] for related models). In view of the known relation between ∆ and the Dirac eigenvalues [12,15], a natural question arises: How is the diquark condensate ψψ reflected in the 3 To evade the sign problem, one has to assume an even number of flavors with degenerate quark masses in the β = 1 and β = 2 cases.…”
mentioning
confidence: 99%
“…In flat space the relativistic BCS/BEC crossover has been studied in [36,37]. From the dual boundary field theory perspective this new ingredient corresponds to an explicit scalar operator of scaling dimension…”
Section: Fermionic Ordering In Holographymentioning
confidence: 99%
“…First, an ordinary BCS-BEC crossover may occur, though the critical temperature in the BEC region no longer tends towards an upper bound, due to relativistic effects. Second, the nonrelativistic BEC state undergoes a transition to a relativisitc BEC (RBEC) state, in which the critical temperature increases to the order of the Fermi energy [15] (see also [16][17][18][19][20] for additional work on the BCS-BEC crossover in relativistic matter).…”
Section: Introductionmentioning
confidence: 99%