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Topologically Charged Vortices at Superconductor-Quantum Hall Interfaces

Enderalp Yakaboylu, Thomas L. Schmidt

Abstract

We explore interface states between a type-II $s$-wave superconductor (SC) and a $ν= 1$ quantum Hall (QH) state. We show that the effective interaction gives rise to two emergent Abelian Higgs fields, representing paired electrons localized at the SC-QH interface. These fields interact with each other in the presence of a Chern-Simons term originating from the QH sector. The Chern-Simons term leads to a topological contribution to the photon mass and imparts a \emph{fractional} topological charge of $e/2$ to the interface vortices. The topological mass modifies the vortex lattice at the interface, while the topological charge leads to formation of vortex quadruplets. We predict that these effects lead to a \emph{topological} Abrikosov lattice at the interface.

Topologically Charged Vortices at Superconductor-Quantum Hall Interfaces

Abstract

We explore interface states between a type-II -wave superconductor (SC) and a quantum Hall (QH) state. We show that the effective interaction gives rise to two emergent Abelian Higgs fields, representing paired electrons localized at the SC-QH interface. These fields interact with each other in the presence of a Chern-Simons term originating from the QH sector. The Chern-Simons term leads to a topological contribution to the photon mass and imparts a \emph{fractional} topological charge of to the interface vortices. The topological mass modifies the vortex lattice at the interface, while the topological charge leads to formation of vortex quadruplets. We predict that these effects lead to a \emph{topological} Abrikosov lattice at the interface.
Paper Structure (7 sections, 112 equations, 2 figures)

This paper contains 7 sections, 112 equations, 2 figures.

Figures (2)

  • Figure 1: Illustration of vortex lattice formation in quadruplets.
  • Figure 2: Numerical vortex solutions \ref{['vortex_ansatz']} (see also Eqs. (83) in SM) for $n=1$ and $e=1$. Parameters: solid lines--$\sqrt{2}\tilde{\kappa}_1=2.35$, $\sqrt{2}\tilde{\kappa}_2=0.56$, $\sqrt{2}\kappa=2.23$, $\delta_2/\delta_1=0.24$; dashed lines--$\sqrt{2}\tilde{\kappa}_1=0.85$, $\sqrt{2}\tilde{\kappa}_2=0.55$, $\sqrt{2}\kappa=1.02$, $\delta_2/\delta_1=0.66$.