Spontaneously broken translational symmetry at edges of high-temperature superconductors: thermodynamics in magnetic field

Abstract

We investigate equilibrium properties, including structure of the order parameter, superflow patterns, and thermodynamics of low-temperature surface phases of layered d_{x^2-y^2}-wave superconductors in magnetic field. At zero external magnetic field, time-reversal symmetry and continuous translational symmetry along the edge are broken spontaneously in a second order phase transition at a temperature $T^{\ast }\approx 0.18T_c$, where $T_c$ is the superconducting transition temperature. At the phase transition there is a jump in the specific heat that scales with the ratio between the edge length $D$ and layer area $\mathcal{A}$ as $(D{\xi }_0/\mathcal{A})\Delta C_d$, where $\Delta C_d$ is the jump in the specific heat at the d-wave superconducting transition and ${\xi }_0$ is the superconducting coherence length. The phase with broken symmetry is characterized by a gauge invariant superfluid momentum ${\mathbf{p}}_s$ that forms a non-trivial planar vector field with a chain of sources and sinks along the edges with a period of approximately $12{\xi }_0$, and saddle point disclinations in the interior. To find out the relative importance of time-reversal and translational symmetry breaking we apply an external field that breaks time-reversal symmetry explicitly. We find that the phase transition into the state with the non-trivial ${\mathbf{p}}_s$ vector field keeps its main signatures, and is still of second order. In the external field, the saddle point disclinations are pushed towards the edges, and thereby a chain of edge motifs are formed, where each motif contains a source, a sink, and a saddle point. Due to a competing paramagnetic response at the edges, the phase transition temperature $T^{\ast }$ is slowly suppressed with increasing magnetic field strength, but the phase with broken symmetry survives into the mixed state.

arXiv comment12 pages, 9 figures

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