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Chiral superconductivity in the alternate stacking compound 4Hb-TaS(2)

Van der Waals materials offer unprecedented control of electronic properties via stacking of different types of two-dimensional materials. A fascinating frontier, largely unexplored, is the stacking of strongly correlated phases of matter. We study 4Hb-TaS(2), which naturally realizes an alternating...

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Detalles Bibliográficos
Autores principales: Ribak, A., Skiff, R. Majlin, Mograbi, M., Rout, P. K., Fischer, M. H., Ruhman, J., Chashka, K., Dagan, Y., Kanigel, A.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Association for the Advancement of Science 2020
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7101217/
https://www.ncbi.nlm.nih.gov/pubmed/32258393
http://dx.doi.org/10.1126/sciadv.aax9480
Descripción
Sumario:Van der Waals materials offer unprecedented control of electronic properties via stacking of different types of two-dimensional materials. A fascinating frontier, largely unexplored, is the stacking of strongly correlated phases of matter. We study 4Hb-TaS(2), which naturally realizes an alternating stacking of 1T-TaS(2) and 1H-TaS(2) structures. The former is a well-known Mott insulator, which has recently been proposed to host a gapless spin-liquid ground state. The latter is a superconductor known to also host a competing charge density wave state. This raises the question of how these two components affect each other when stacked together. We find a superconductor with a T(c) of 2.7 Kelvin and anomalous properties, of which the most notable one is a signature of time-reversal symmetry breaking, abruptly appearing at the superconducting transition. This observation is consistent with a chiral superconducting state.