Theory of 2D superconductor with broken inversion symmetry
arXiv:cond-mat/0701698 · doi:10.1103/PhysRevB.76.014522
Abstract
A detailed theory of a phase diagram of a 2D surface superconductor in a parallel magnetic field is presented. A spin-orbital interaction of the Rashba type is known to produce at a high magnetic field (and in the absence of impurities) an inhomogeneous superconductive phase similar to the Larkin-Ovchinnikov-Fulde-Ferrel (LOFF) state with an order parameter . We consider the case of a strong Rashba interaction with the spin-orbital splitting much larger than the superconductive gap , and show that at low temperatures the LOFF-type state is separated from the usual homogeneous state by a first-order phase transition line. At higher temperatures another inhomogeneous state with intervenes between the uniform BCS state and the LOFF-like state at . The modulation vector in both phases is of the order of . The superfluid density vanishes in the region around the second-order transition line between the BCS state and the new ``helical'' state. Non-magnetic impurities suppress both inhomogeneous states, and eliminate them completely at . However, once an account is made of the next-order term over the small parameter , a relatively long-wave helical modulation with is found to develop from the BCS state. This long-wave modulation is stable with respect to disorder. In addition, we predict that unusual vortex defects with a continuous core exist near the phase boundary between the helical and the LOFF-like states. In particular, in the LOFF-like state these defects may carry a half-integer flux.
23 pages, 14 figures
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