Möller, Gunnar, Cooper, N R, Gurarie, V (2011) Structure and consequences of vortex-core states in p-wave superfluids. Physical Review B: Condensed Matter and Materials Physics, 83 . 014513. ISSN 0163-1829. (doi:10.1103/PhysRevB.83.014513) (KAR id:55590)
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Official URL: http://dx.doi.org/10.1103/PhysRevB.83.014513 |
Abstract
It is now well established that in two-dimensional chiral $p$-wave paired superfluids, the vortices carry zero-energy
modes which obey non-abelian exchange statistics and can potentially be used for topological quantum computation.
In such superfluids there may also exist other excitations below the bulk gap inside the cores of vortices.
We study the properties of these subgap states, and argue that their
presence affects the topological protection of the zero modes.
In conventional superconductors where the chemical potential is of the order of the Fermi energy
of a non-interacting Fermi gas, there is a large number of subgap states and the mini-gap
towards the lowest of these states is a small fraction of the Fermi energy. It is therefore difficult
to cool the system to below the mini-gap and at experimentally available temperatures, transitions
between the subgap states, including the zero modes, will occur and can alter the quantum
states of the zero-modes. Consequently, qubits defined uniquely in terms of the zero-modes
do not remain coherent.
We show that compound qubits involving the zero-modes and the parity of the occupation number
of the subgap states on each vortex are still well defined. However, practical schemes taking into
account all subgap states would nonetheless be difficult to achieve.
We propose to avoid this difficulty by working in the regime of small chemical potential $\mu$, near the transition
to a strongly paired phase, where the number of subgap states is reduced. We develop the theory to describe
this regime of strong pairing interactions and we show how the subgap states are ultimately absorbed into the bulk gap.
Since the bulk gap also vanishes as $\mu\to 0$ there is an optimum value $\mu_c$ which maximises the combined gap.
We propose cold atomic gases as candidate systems where the regime of strong interactions can be explored,
and explicitly evaluate $\mu_c$ in a Feshbach resonant $^{40}$K gas.
Item Type: | Article |
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DOI/Identification number: | 10.1103/PhysRevB.83.014513 |
Uncontrolled keywords: | Physics of Quantum Materials, superfluid, BEC-BCS crossover, p-wave, superconductor, vortices, subgap state, Majorana, topological quantum computation, Physics of Quantum Materials |
Subjects: |
Q Science > QC Physics > QC173.45 Condensed Matter Q Science > QC Physics > QC174.12 Quantum theory |
Divisions: | Divisions > Division of Natural Sciences > Physics and Astronomy |
Depositing User: | Gunnar Moeller |
Date Deposited: | 29 Sep 2016 14:49 UTC |
Last Modified: | 16 Nov 2021 10:23 UTC |
Resource URI: | https://kar.kent.ac.uk/id/eprint/55590 (The current URI for this page, for reference purposes) |
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