2014
DOI: 10.1007/s10948-014-2906-4
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Superconductivity, Charge Orderings, Magnetism, and Their Phase Separations in the Ground State of Lattice Models of Superconductor with Very Short Coherence Length

Abstract: We present the ground state results for lattice models of superconductor (SC) with extremely short coherence length, which also involve the interplay with charge (CO) and (anti-)ferromagnetic orderings. Our preliminary results at zero temperature (derived by means of the variational approach which treats the on-site interaction term exactly and the intersite interactions within the mean field approximation, exact in d → +∞), yields that the SC phase can coexist with the CO or magnetic (M) phases in states with… Show more

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Cited by 16 publications
(22 citation statements)
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References 46 publications
(103 reference statements)
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“…Similar as in previous case all transitions lines merge at a bicritical point B. Moreover, at T = 0 the PS:SC/CO state is degenerated with the MIX2:SC/CO phase (a coexistence of SC and CO in homogeneous phase, ∆q, n Q = 0), but at any T > 0 that degeneration is removed [8,9,29]. With increasing W > 0, the B-point moves along the SCNO boundary toward larger |μ| (|1 − n|).…”
Section: Superconductivity and Charge Orderingssupporting
confidence: 77%
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“…Similar as in previous case all transitions lines merge at a bicritical point B. Moreover, at T = 0 the PS:SC/CO state is degenerated with the MIX2:SC/CO phase (a coexistence of SC and CO in homogeneous phase, ∆q, n Q = 0), but at any T > 0 that degeneration is removed [8,9,29]. With increasing W > 0, the B-point moves along the SCNO boundary toward larger |μ| (|1 − n|).…”
Section: Superconductivity and Charge Orderingssupporting
confidence: 77%
“…also Refs. [8,9,24]) and they do not change with decreasing W < 0. The rst-order NONO transition line (vertical one for xedμ = 0) ends at critical point C located at kBT /WQ = 0.5.…”
Section: Superconductivity and Charge Orderingsmentioning
confidence: 90%
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“…In this section we present a brief review of the zerotemperature results for the atomic limit (t = 0) of model (1) derived in [22][23][24][25]. For large U, |J| t the effective magnetic interaction in model (1) can be obtained as K eff ≈ −4t 2 /(U − |J|).…”
Section: Results In the Atomic Limitmentioning
confidence: 99%