2020
DOI: 10.1016/j.ppnp.2019.103739
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BCS–BEC crossover in cold atomic and in nuclear systems

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Cited by 82 publications
(86 citation statements)
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“…In this paper, we elucidate pairing fluctuation effects in 1D Gaudin-Yang Fermi gas at finite temperature within the diagrammatic approach, which has successfully been applied to higher-dimensional systems [6,9,11,12,14]. Our numerical results of the number density show an excellent agreement with the recent QMC results [66].…”
Section: Introductionsupporting
confidence: 64%
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“…In this paper, we elucidate pairing fluctuation effects in 1D Gaudin-Yang Fermi gas at finite temperature within the diagrammatic approach, which has successfully been applied to higher-dimensional systems [6,9,11,12,14]. Our numerical results of the number density show an excellent agreement with the recent QMC results [66].…”
Section: Introductionsupporting
confidence: 64%
“…3(c2) since the low-energy pole in (q, iν ) becomes close to q = 0 and gives a strong particle-hole coupling, one can clearly see the pseudogap accompanying with particlehole branches. Intuitively, this pseudogap structure can be understood from the so-called static approximation where [12,14]. Here, 2 pg = −T q,iν (q, iν ) is called the pseudogap parameter which characterizes its size in A(p, ω) as well as ρ(ω).…”
Section: Resultsmentioning
confidence: 99%
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“…One of the exciting topics in the two-band BCS-BEC crossover is the existence of pseudogaps in the single-particle excitation in the normal state (for reviews discussing the pseudogap, see [27][28][29]). While several experiments for FeSe report signals of pseudogaps and preformed Cooper pairs [30][31][32][33], a recent scanning tunneling spectroscopy (STS) measurement did not observe a pseudogap behavior even in the crossover regime of the BCS-BEC crossover [34].…”
Section: Introductionmentioning
confidence: 99%