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Sökning: onr:"swepub:oai:lup.lub.lu.se:26e06c5d-4ea1-4d68-b7a7-5e154f4a982d" > Current-driven insu...

LIBRIS Formathandbok  (Information om MARC21)
FältnamnIndikatorerMetadata
00003870naa a2200505 4500
001oai:lup.lub.lu.se:26e06c5d-4ea1-4d68-b7a7-5e154f4a982d
003SwePub
008240112s2023 | |||||||||||000 ||eng|
024a https://lup.lub.lu.se/record/26e06c5d-4ea1-4d68-b7a7-5e154f4a982d2 URI
024a https://doi.org/10.1103/PhysRevB.108.L1611052 DOI
040 a (SwePub)lu
041 a engb eng
042 9 SwePub
072 7a art2 swepub-publicationtype
072 7a ref2 swepub-contenttype
100a Curcio, Davideu Aarhus University4 aut
2451 0a Current-driven insulator-to-metal transition without Mott breakdown in Ca2RuO4
264 1c 2023
520 a The electrical control of a material's conductivity is at the heart of modern electronics. Conventionally, this control is achieved by tuning the density of mobile charge carriers. A completely different approach is possible in Mott insulators such as Ca2RuO4, where an insulator-to-metal transition (IMT) can be induced by a weak electric field or current. While the driving force of the IMT is poorly understood, it has been thought to be a breakdown of the Mott state. Using in operando angle-resolved photoemission spectroscopy, we show that this is not the case: The current-induced conductivity is caused by the formation of in-gap states with only a minor reorganization of the Mott state. Electronic structure calculations show that these in-gap states form at the boundaries of structural domains that emerge during the IMT. At such boundaries, the overall gap is drastically reduced, even if the structural difference between the domains is small and the individual domains retain their Mott character. The inhomogeneity of the sample is thus key to understanding the IMT, as it leads to a nonequilibrium semimetallic state that forms at the interface of Mott domains.
650 7a NATURVETENSKAPx Fysikx Den kondenserade materiens fysik0 (SwePub)103042 hsv//swe
650 7a NATURAL SCIENCESx Physical Sciencesx Condensed Matter Physics0 (SwePub)103042 hsv//eng
700a Sanders, Charlotte E.4 aut
700a Chikina, Allau Aarhus University4 aut
700a Lund, Henriette E.u Aarhus University4 aut
700a Bianchi, Marcou Aarhus University4 aut
700a Granata, Veronicau University of Salerno4 aut
700a Cannavacciuolo, Marcou University of Salerno4 aut
700a Cuono, Giuseppeu Institute of Physics of the Polish Academy of Sciences4 aut
700a Autieri, Carmineu Institute of Physics of the Polish Academy of Sciences4 aut
700a Forte, Filomena4 aut
700a Avallone, Guerinou University of Salerno4 aut
700a Romano, Alfonsou University of Salerno4 aut
700a Cuoco, Mario4 aut
700a Dudin, Pavelu Synchrotron SOLEIL4 aut
700a Avila, Joseu Synchrotron SOLEIL4 aut
700a Polley, Craigu Lund University,Lunds universitet,MAX IV, Bloch,MAX IV, Spektroskopi I,MAX IV, Vetenskapsavdelning,MAX IV-laboratoriet,MAX IV, Bloch,MAX IV,Spectroscopy I,MAX IV, Science division,MAX IV Laboratory4 aut0 (Swepub:lu)cr4837po
700a Balasubramanian, Thiagarajanu Lund University,Lunds universitet,MAX IV, Bloch,MAX IV, Spektroskopi I,MAX IV, Vetenskapsavdelning,MAX IV-laboratoriet,MAX IV, Bloch,MAX IV,Spectroscopy I,MAX IV, Science division,MAX IV Laboratory4 aut0 (Swepub:lu)maxl-bth
700a Fittipaldi, Rosalba4 aut
700a Vecchione, Antonio4 aut
700a Hofmann, Philipu Aarhus University4 aut
710a Aarhus Universityb University of Salerno4 org
773t Physical Review Bg 108:16q 108:16x 2469-9950
856u http://dx.doi.org/10.1103/PhysRevB.108.L161105y FULLTEXT
8564 8u https://lup.lub.lu.se/record/26e06c5d-4ea1-4d68-b7a7-5e154f4a982d
8564 8u https://doi.org/10.1103/PhysRevB.108.L161105

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