Biot-Savart correlations in layered superconductors
arXiv:0902.1547 · doi:10.1103/PhysRevB.79.174528
Abstract
We discuss the superconductor to normal phase transition in an infinite-layered type-II superconductor in the limit where the Josephson coupling between layers is negligible. We model each layer as a neutral gas of thermally excited pancake vortices. We assume the dominant interaction between vortices in the same and in different layers is the electromagnetic interaction between the screening currents induced by these vortices. Our main result, obtained by exactly solving the leading order renormalization group flow, is that the phase transition in this model is a Kosterlitz--Thouless transition despite being a three--dimensional system. While the transition itself is driven by the unbinding of two-dimensional pancake vortices, an RG analysis of the low temperature phase and a mean-field theory of the high temperature phase reveal that both phases possess three-dimensional correlations. An experimental consequence of this is that the jump in the measured in-plane superfluid stiffness, which is a universal quantity in 2d Kosterlitz-Thouless theory, will receive a small non--universal correction (of order 1% in BiSrCaCuO). This overall picture places some claims expressed in the literature on a more secure analytical footing and also resolves some conflicting views.
16 pages, 2 figures; minor typos corrected, references added
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Cited by in corpus (8)
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- Uniaxial linear resistivity of superconducting La(1.905)Ba(0.095)CuO(4) induced by an external magnetic field
- Tuning from failed superconductor to failed insulator with magnetic field
- Berezinskii-Kosterlitz-Thouless Transition in Heavy Fermion Superlattices
- Evolution of superconducting correlations within magnetic-field-decoupled CuO(2) layers of La(1.905)Ba(0.095)CuO(4)
- Evidence for Correlated Dynamics near the Berezinskii-Kosterlitz-Thouless-like Transition in Highly Underdoped LaSrCuO
- Transport Properties of Stripe-Ordered High Tc Cuprates