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arxiv: 1603.05207 · v1 · pith:W5DLKJ4Bnew · submitted 2016-03-16 · ❄️ cond-mat.supr-con · cond-mat.mes-hall· cond-mat.mtrl-sci· cond-mat.str-el

Spin-valley locking in the normal state of a transition-metal dichalocogenide superconductor

classification ❄️ cond-mat.supr-con cond-mat.mes-hallcond-mat.mtrl-scicond-mat.str-el
keywords statetmdcschargenaturenbsenormalphasesspin
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The metallic transition-metal dichalcogenides (TMDCs) are benchmark systems for studying and controlling intertwined electronic orders in solids, with superconductivity developing upon cooling from a charge density wave state. The interplay between such phases is thought to play a critical role in the unconventional superconductivity of cuprates, Fe-based, and heavy-fermion systems, yet even for the more moderately-correlated TMDCs, their nature and origins have proved highly controversial. Here, we study a prototypical example, $2H$-NbSe$_2$, by spin- and angle-resolved photoemission and first-principles theory. We find that the normal state, from which its hallmark collective phases emerge, is characterised by quasiparticles whose spin is locked to their valley pseudospin. This results from a combination of strong spin-orbit interactions and local inversion symmetry breaking. Non-negligible interlayer coupling further drives a rich three-dimensional momentum-dependence of the underlying Fermi surface spin texture. Together, these findings necessitate a fundamental re-investigation of the nature of charge order and superconducting pairing in NbSe$_2$ and related TMDCs.

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