2009
DOI: 10.1103/physrevb.80.214515
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Dissipation-driven phase transitions in superconducting wires

Abstract: We report on the reinforcement of superconductivity in a system consisting of a narrow superconducting wire weakly coupled to a diffusive metallic film. We analyze the effective phase-only action of the system by a perturbative renormalization group and a self-consistent variational approach to obtain the critical points and phases at T = 0. We predict a quantum phase transition toward a superconducting phase with long-range order as a function of the wire stiffness and coupling to the metal. We discuss implic… Show more

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Cited by 12 publications
(18 citation statements)
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References 49 publications
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“…Interestingly, recent theoretical works have shown the possibility to stabilize a 1D SC through a weak coupling to a dissipative environment [4][5][6][7][8][9] that suppresses fluctuations and restore phase coherence 10 . Experimentally, restoration of phase coherence has been recently observed in thin Zn 11,12 and Al 13 nanowires by increasing the coupling of the wire to dissipative electrodes.…”
mentioning
confidence: 99%
See 1 more Smart Citation
“…Interestingly, recent theoretical works have shown the possibility to stabilize a 1D SC through a weak coupling to a dissipative environment [4][5][6][7][8][9] that suppresses fluctuations and restore phase coherence 10 . Experimentally, restoration of phase coherence has been recently observed in thin Zn 11,12 and Al 13 nanowires by increasing the coupling of the wire to dissipative electrodes.…”
mentioning
confidence: 99%
“…0 stands for the average with respect to the trial action S 0 . Minimizing F var with respect to g 0 (q), i.e., ∂F var /∂g 0 (q) = 0, results in a self-consistent equation for g 0 (q) 3,4,6 . In the regime 1/2 < α < 3/2, L → ∞, T → 0, an approximate solution, asymptotically correct in the limit k → 0, is given by the expression…”
mentioning
confidence: 99%
“…We adopt a Gaussian ansatz S 0 = 1 2βL ∑ q g −1 0 (q) θ * q θ q for the Euclidean action of the system, with q = (k, −ω m ), ω m = 2πT m being the bosonic Matsubara frequencies at temperature T [16], and the functions g −1 0 (q) being unknown variational parameters which must be chosen to minimize the variational free energy F var = F 0 + T S − S 0 0 . Then we obtain a self-consistent equation for g 0 (q) [4,8,17,18] …”
Section: Bosonization Analysis Of the Hard-core Boson Modelmentioning
confidence: 99%
“…For SC LRO to be stabilized, a finite η > 0 is needed. A selfconsistent equation for η [17][18][19] is obtained by combining (5) with (4). In the limit of λ → 0, a solution with η > 0 exists only for α < 3/2 − 1/(4K) [8].…”
Section: Bosonization Analysis Of the Hard-core Boson Modelmentioning
confidence: 99%
“…23,24 Therefore, a better understanding of the screening effects occurring in superconducting wires and the consequences to their superconducting properties is needed. This issue is particularly relevant to recent theoretical 13,25,26 and experimental 27,28 works showing evidence of stabilization of superconductivity in low-dimensional systems due to the presence of tunneling contacts with normal metallic leads, which suppress fluctuations of the superconducting order parameter. It would be desirable to investigate to what extent the same leads introduce additional sources of dissipation prejudicial to superconductivity.…”
Section: Introductionmentioning
confidence: 98%