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dc.contributor.author
Hepting, M.  
dc.contributor.author
Boyko, T. D.  
dc.contributor.author
Zimmermann, V.  
dc.contributor.author
Bejas, Matias Hector  
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Suyolcu, Y. E.  
dc.contributor.author
Puphal, P.  
dc.contributor.author
Green, R. J.  
dc.contributor.author
Zinni, Luciano Sebastian  
dc.contributor.author
Kim, J.  
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Casa, D.  
dc.contributor.author
Upton, M. H.  
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Wong, D.  
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Schulz, C.  
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Bartkowiak, M.  
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Habicht, K.  
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Pomjakushina, E.  
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Cristiani, G.  
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Logvenov, G.  
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Minola, M.  
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Yamase, H.  
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Greco, Andres Francisco  
dc.contributor.author
Keimer, B.  
dc.date.available
2025-12-03T10:00:40Z  
dc.date.issued
2023-06  
dc.identifier.citation
Hepting, M.; Boyko, T. D.; Zimmermann, V.; Bejas, Matias Hector; Suyolcu, Y. E.; et al.; Evolution of plasmon excitations across the phase diagram of the cuprate superconductor La2−xSrxCuO4; American Physical Society; Physical Review B; 107; 21; 6-2023; 1-18  
dc.identifier.issn
2469-9950  
dc.identifier.uri
http://hdl.handle.net/11336/276609  
dc.description.abstract
We use resonant inelastic x-ray scattering (RIXS) at the O K- and Cu K-edges to investigate the doping dependence and temperature dependence of low-energy plasmon excitations in La2-xSrxCuO4. We observe a monotonic increase of the energy scale of the plasmons with increasing doping x in the underdoped regime, whereas a saturation occurs above optimal doping x≳0.16 and persists at least up to x=0.4. Furthermore, we find that the plasmon excitations show only a marginal temperature dependence, and possible effects due to the superconducting transition and the onset of strange metal behavior are either absent or below the detection limit of our experiment. Taking into account the strongly correlated character of the cuprates, we show that layered t-J-V model calculations accurately capture the increase of the plasmon energy in the underdoped regime. However, the computed plasmon energy continues to increase even for doping levels above x≳0.16, which is distinct from the experimentally observed saturation and reaches a broad maximum around x=0.55. We discuss whether possible lattice disorder in overdoped samples, a renormalization of the electronic correlation strength at high dopings, or an increasing relevance of nonplanar Cu and O orbitals could be responsible for the discrepancy between experiment and theory for doping levels above x=0.16.  
dc.format
application/pdf  
dc.language.iso
eng  
dc.publisher
American Physical Society  
dc.rights
info:eu-repo/semantics/openAccess  
dc.rights.uri
https://creativecommons.org/licenses/by/2.5/ar/  
dc.subject
PLASMONS  
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SUPERCONDUCTIVITY  
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RESONANT INELASTIC X-RAY SCATTERING  
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T-J MODEL  
dc.subject.classification
Física de los Materiales Condensados  
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Ciencias Físicas  
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CIENCIAS NATURALES Y EXACTAS  
dc.title
Evolution of plasmon excitations across the phase diagram of the cuprate superconductor La2−xSrxCuO4  
dc.type
info:eu-repo/semantics/article  
dc.type
info:ar-repo/semantics/artículo  
dc.type
info:eu-repo/semantics/publishedVersion  
dc.date.updated
2024-12-09T09:24:34Z  
dc.identifier.eissn
2469-9969  
dc.journal.volume
107  
dc.journal.number
21  
dc.journal.pagination
1-18  
dc.journal.pais
Estados Unidos  
dc.journal.ciudad
Maryland  
dc.description.fil
Fil: Hepting, M.. Max-Planck-Institute for Solid State Research; Alemania  
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Fil: Boyko, T. D.. Centre Canadien de Rayonnement Synchrotron; Canadá  
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Fil: Zimmermann, V.. Max-Planck-Institute for Solid State Research; Alemania  
dc.description.fil
Fil: Bejas, Matias Hector. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - Rosario. Instituto de Física de Rosario. Universidad Nacional de Rosario. Instituto de Física de Rosario; Argentina  
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Fil: Suyolcu, Y. E.. Max-Planck-Institute for Solid State Research; Alemania  
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Fil: Puphal, P.. Max-Planck-Institute for Solid State Research; Alemania  
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Fil: Green, R. J.. University of British Columbia; Canadá. University of Saskatchewan; Canadá  
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Fil: Zinni, Luciano Sebastian. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - Rosario; Argentina. Universidad Nacional de Rosario. Facultad de Ciencias Exactas, Ingeniería y Agrimensura; Argentina  
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Fil: Kim, J.. Argonne National Laboratory; Estados Unidos  
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Fil: Casa, D.. Argonne National Laboratory; Estados Unidos  
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Fil: Upton, M. H.. Argonne National Laboratory; Estados Unidos  
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Fil: Wong, D.. Helmholtz-Zentrum Berlin für Materialien und Energie; Alemania  
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Fil: Schulz, C.. Helmholtz-Zentrum Berlin für Materialien und Energie; Alemania  
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Fil: Bartkowiak, M.. Helmholtz-Zentrum Berlin für Materialien und Energie; Alemania  
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Fil: Habicht, K.. Universitat Potsdam; Alemania. Helmholtz-Zentrum Berlin für Materialien und Energie; Alemania  
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Fil: Pomjakushina, E.. Paul Scherrer Institut; Suiza  
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Fil: Cristiani, G.. Max Planck Institute For Solid State Research; Alemania  
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Fil: Logvenov, G.. Max Planck Institute For Solid State Research; Alemania  
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Fil: Minola, M.. Max Planck Institute For Solid State Research; Alemania  
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Fil: Yamase, H.. Tsukuba University. National Institute For Materials Science; Japón  
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Fil: Greco, Andres Francisco. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - Rosario. Instituto de Física de Rosario. Universidad Nacional de Rosario. Instituto de Física de Rosario; Argentina  
dc.description.fil
Fil: Keimer, B.. Max Planck Institute For Solid State Research; Alemania  
dc.journal.title
Physical Review B  
dc.relation.alternativeid
info:eu-repo/semantics/altIdentifier/url/https://journals.aps.org/prb/abstract/10.1103/PhysRevB.107.214516  
dc.relation.alternativeid
info:eu-repo/semantics/altIdentifier/doi/https://doi.org/10.1103/PhysRevB.107.214516