2017
DOI: 10.48550/arxiv.1710.10575
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Gauge Topological Nature of the Superconductor-Insulator Transition

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“…We start by showing how dual superconducting and superinsulating states can be understood from the uncertainty principle, ∆N∆ϕ 1 between the number of charges, N = 2|Ψ| 2 , and the phase ϕ of the Cooper pairs quantum field Ψ = N exp(iϕ), bound by the commutation relation [N, ϕ] = i [15,20]. At zero temperature, superconductors correspond to fixed ϕ, hence indefinite N. Inversely, fixed N and indefinite ϕ characterizes the superinsulating state.…”
Section: Action In Two-dimensional Systemsmentioning
confidence: 99%
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“…We start by showing how dual superconducting and superinsulating states can be understood from the uncertainty principle, ∆N∆ϕ 1 between the number of charges, N = 2|Ψ| 2 , and the phase ϕ of the Cooper pairs quantum field Ψ = N exp(iϕ), bound by the commutation relation [N, ϕ] = i [15,20]. At zero temperature, superconductors correspond to fixed ϕ, hence indefinite N. Inversely, fixed N and indefinite ϕ characterizes the superinsulating state.…”
Section: Action In Two-dimensional Systemsmentioning
confidence: 99%
“…Here µ P is the magnetic permeability and ε P is the electric permittivity [20], which define the speed of light v c = 1/ √ µ P ε P in the material. The two coupling constants, e 2 q = e 2 /d and e 2 v = π 2 /(e 2 λ ⊥ ) are the characteristic energies of a charge and a vortex in the film, respectively [20]. Here d is the thickness of the film, λ ⊥ = λ 2 L /d is the Pearl length, and λ L is the London length of the bulk.…”
Section: Action In Two-dimensional Systemsmentioning
confidence: 99%