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arxiv: 1307.3240 · v2 · pith:F6252UVEnew · submitted 2013-07-11 · ❄️ cond-mat.supr-con · cond-mat.mes-hall· cond-mat.str-el· hep-th· quant-ph

Axionic superconductivity in three dimensional doped narrow gap semiconductors

classification ❄️ cond-mat.supr-con cond-mat.mes-hallcond-mat.str-elhep-thquant-ph
keywords mathrmstateanomalousaxionicb-phasedimensionaldopednarrow
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We consider the competition between the conventional s-wave and the triplet Balian-Werthamer or the B-phase pairings in the doped three dimensional narrow gap semiconductors, such as $\mathrm{Cu}_x\mathrm{Bi}_2\mathrm{Se}_3$ and $\mathrm{Sn}_{1-x}\mathrm{In}_x\mathrm{Te}$. When the coupling constants of the two contending channels are comparable, we find a simultaneously time-reversal and parity violating $p + is$ state at low temperatures, which provides an example of dynamic axionic state of matter. In contradistinction to the time-reversal invariant, topological B-phase, the $p + is$ state possesses gapped Majorana fermions as the surface Andreev bound states, which give rise to an anomalous surface thermal Hall effect. The anomalous gravitational and electrodynamic responses of the $p+is$ state can be described by the $\theta$ vacuum structure, where $\theta \neq 0$ or $\pi$.

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