Evolution of plasmon excitations across the phase diagram of the cuprate superconductor La2−xSrxCuO4
- Autores
- Hepting, M.; Boyko, T. D.; Zimmermann, V.; Bejas, Matias Hector; Suyolcu, Y. E.; Puphal, P.; Green, R. J.; Zinni, Luciano Sebastian; Kim, J.; Casa, D.; Upton, M. H.; Wong, D.; Schulz, C.; Bartkowiak, M.; Habicht, K.; Pomjakushina, E.; Cristiani, G.; Logvenov, G.; Minola, M.; Yamase, H.; Greco, Andres Francisco; Keimer, B.
- Año de publicación
- 2023
- Idioma
- inglés
- Tipo de recurso
- artículo
- Estado
- versión publicada
- Descripción
- 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.
Fil: Hepting, M.. Max-Planck-Institute for Solid State Research; Alemania
Fil: Boyko, T. D.. Centre Canadien de Rayonnement Synchrotron; Canadá
Fil: Zimmermann, V.. Max-Planck-Institute for Solid State Research; Alemania
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
Fil: Suyolcu, Y. E.. Max-Planck-Institute for Solid State Research; Alemania
Fil: Puphal, P.. Max-Planck-Institute for Solid State Research; Alemania
Fil: Green, R. J.. University of British Columbia; Canadá. University of Saskatchewan; Canadá
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
Fil: Kim, J.. Argonne National Laboratory; Estados Unidos
Fil: Casa, D.. Argonne National Laboratory; Estados Unidos
Fil: Upton, M. H.. Argonne National Laboratory; Estados Unidos
Fil: Wong, D.. Helmholtz-Zentrum Berlin für Materialien und Energie; Alemania
Fil: Schulz, C.. Helmholtz-Zentrum Berlin für Materialien und Energie; Alemania
Fil: Bartkowiak, M.. Helmholtz-Zentrum Berlin für Materialien und Energie; Alemania
Fil: Habicht, K.. Universitat Potsdam; Alemania. Helmholtz-Zentrum Berlin für Materialien und Energie; Alemania
Fil: Pomjakushina, E.. Paul Scherrer Institut; Suiza
Fil: Cristiani, G.. Max Planck Institute For Solid State Research; Alemania
Fil: Logvenov, G.. Max Planck Institute For Solid State Research; Alemania
Fil: Minola, M.. Max Planck Institute For Solid State Research; Alemania
Fil: Yamase, H.. Tsukuba University. National Institute For Materials Science; Japón
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
Fil: Keimer, B.. Max Planck Institute For Solid State Research; Alemania - Materia
-
PLASMONS
SUPERCONDUCTIVITY
RESONANT INELASTIC X-RAY SCATTERING
T-J MODEL - Nivel de accesibilidad
- acceso abierto
- Condiciones de uso
- https://creativecommons.org/licenses/by/2.5/ar/
- Repositorio
.jpg)
- Institución
- Consejo Nacional de Investigaciones Científicas y Técnicas
- OAI Identificador
- oai:ri.conicet.gov.ar:11336/276609
Ver los metadatos del registro completo
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Evolution of plasmon excitations across the phase diagram of the cuprate superconductor La2−xSrxCuO4Hepting, M.Boyko, T. D.Zimmermann, V.Bejas, Matias HectorSuyolcu, Y. E.Puphal, P.Green, R. J.Zinni, Luciano SebastianKim, J.Casa, D.Upton, M. H.Wong, D.Schulz, C.Bartkowiak, M.Habicht, K.Pomjakushina, E.Cristiani, G.Logvenov, G.Minola, M.Yamase, H.Greco, Andres FranciscoKeimer, B.PLASMONSSUPERCONDUCTIVITYRESONANT INELASTIC X-RAY SCATTERINGT-J MODELhttps://purl.org/becyt/ford/1.3https://purl.org/becyt/ford/1We 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.Fil: Hepting, M.. Max-Planck-Institute for Solid State Research; AlemaniaFil: Boyko, T. D.. Centre Canadien de Rayonnement Synchrotron; CanadáFil: Zimmermann, V.. Max-Planck-Institute for Solid State Research; AlemaniaFil: 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; ArgentinaFil: Suyolcu, Y. E.. Max-Planck-Institute for Solid State Research; AlemaniaFil: Puphal, P.. Max-Planck-Institute for Solid State Research; AlemaniaFil: Green, R. J.. University of British Columbia; Canadá. University of Saskatchewan; CanadáFil: 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; ArgentinaFil: Kim, J.. Argonne National Laboratory; Estados UnidosFil: Casa, D.. Argonne National Laboratory; Estados UnidosFil: Upton, M. H.. Argonne National Laboratory; Estados UnidosFil: Wong, D.. Helmholtz-Zentrum Berlin für Materialien und Energie; AlemaniaFil: Schulz, C.. Helmholtz-Zentrum Berlin für Materialien und Energie; AlemaniaFil: Bartkowiak, M.. Helmholtz-Zentrum Berlin für Materialien und Energie; AlemaniaFil: Habicht, K.. Universitat Potsdam; Alemania. Helmholtz-Zentrum Berlin für Materialien und Energie; AlemaniaFil: Pomjakushina, E.. Paul Scherrer Institut; SuizaFil: Cristiani, G.. Max Planck Institute For Solid State Research; AlemaniaFil: Logvenov, G.. Max Planck Institute For Solid State Research; AlemaniaFil: Minola, M.. Max Planck Institute For Solid State Research; AlemaniaFil: Yamase, H.. Tsukuba University. National Institute For Materials Science; JapónFil: 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; ArgentinaFil: Keimer, B.. Max Planck Institute For Solid State Research; AlemaniaAmerican Physical Society2023-06info:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersionhttp://purl.org/coar/resource_type/c_6501info:ar-repo/semantics/articuloapplication/pdfapplication/pdfapplication/pdfapplication/pdfhttp://hdl.handle.net/11336/276609Hepting, 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; 1-182469-99502469-9969CONICET DigitalCONICETenginfo:eu-repo/semantics/altIdentifier/url/https://journals.aps.org/prb/abstract/10.1103/PhysRevB.107.214516info:eu-repo/semantics/altIdentifier/doi/10.1103/PhysRevB.107.214516info:eu-repo/semantics/openAccesshttps://creativecommons.org/licenses/by/2.5/ar/reponame:CONICET Digital (CONICET)instname:Consejo Nacional de Investigaciones Científicas y Técnicas2025-12-23T14:35:42Zoai:ri.conicet.gov.ar:11336/276609instacron:CONICETInstitucionalhttp://ri.conicet.gov.ar/Organismo científico-tecnológicoNo correspondehttp://ri.conicet.gov.ar/oai/requestdasensio@conicet.gov.ar; lcarlino@conicet.gov.arArgentinaNo correspondeNo correspondeNo correspondeopendoar:34982025-12-23 14:35:43.228CONICET Digital (CONICET) - Consejo Nacional de Investigaciones Científicas y Técnicasfalse |
| dc.title.none.fl_str_mv |
Evolution of plasmon excitations across the phase diagram of the cuprate superconductor La2−xSrxCuO4 |
| title |
Evolution of plasmon excitations across the phase diagram of the cuprate superconductor La2−xSrxCuO4 |
| spellingShingle |
Evolution of plasmon excitations across the phase diagram of the cuprate superconductor La2−xSrxCuO4 Hepting, M. PLASMONS SUPERCONDUCTIVITY RESONANT INELASTIC X-RAY SCATTERING T-J MODEL |
| title_short |
Evolution of plasmon excitations across the phase diagram of the cuprate superconductor La2−xSrxCuO4 |
| title_full |
Evolution of plasmon excitations across the phase diagram of the cuprate superconductor La2−xSrxCuO4 |
| title_fullStr |
Evolution of plasmon excitations across the phase diagram of the cuprate superconductor La2−xSrxCuO4 |
| title_full_unstemmed |
Evolution of plasmon excitations across the phase diagram of the cuprate superconductor La2−xSrxCuO4 |
| title_sort |
Evolution of plasmon excitations across the phase diagram of the cuprate superconductor La2−xSrxCuO4 |
| dc.creator.none.fl_str_mv |
Hepting, M. Boyko, T. D. Zimmermann, V. Bejas, Matias Hector Suyolcu, Y. E. Puphal, P. Green, R. J. Zinni, Luciano Sebastian Kim, J. Casa, D. Upton, M. H. Wong, D. Schulz, C. Bartkowiak, M. Habicht, K. Pomjakushina, E. Cristiani, G. Logvenov, G. Minola, M. Yamase, H. Greco, Andres Francisco Keimer, B. |
| author |
Hepting, M. |
| author_facet |
Hepting, M. Boyko, T. D. Zimmermann, V. Bejas, Matias Hector Suyolcu, Y. E. Puphal, P. Green, R. J. Zinni, Luciano Sebastian Kim, J. Casa, D. Upton, M. H. Wong, D. Schulz, C. Bartkowiak, M. Habicht, K. Pomjakushina, E. Cristiani, G. Logvenov, G. Minola, M. Yamase, H. Greco, Andres Francisco Keimer, B. |
| author_role |
author |
| author2 |
Boyko, T. D. Zimmermann, V. Bejas, Matias Hector Suyolcu, Y. E. Puphal, P. Green, R. J. Zinni, Luciano Sebastian Kim, J. Casa, D. Upton, M. H. Wong, D. Schulz, C. Bartkowiak, M. Habicht, K. Pomjakushina, E. Cristiani, G. Logvenov, G. Minola, M. Yamase, H. Greco, Andres Francisco Keimer, B. |
| author2_role |
author author author author author author author author author author author author author author author author author author author author author |
| dc.subject.none.fl_str_mv |
PLASMONS SUPERCONDUCTIVITY RESONANT INELASTIC X-RAY SCATTERING T-J MODEL |
| topic |
PLASMONS SUPERCONDUCTIVITY RESONANT INELASTIC X-RAY SCATTERING T-J MODEL |
| purl_subject.fl_str_mv |
https://purl.org/becyt/ford/1.3 https://purl.org/becyt/ford/1 |
| dc.description.none.fl_txt_mv |
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. Fil: Hepting, M.. Max-Planck-Institute for Solid State Research; Alemania Fil: Boyko, T. D.. Centre Canadien de Rayonnement Synchrotron; Canadá Fil: Zimmermann, V.. Max-Planck-Institute for Solid State Research; Alemania 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 Fil: Suyolcu, Y. E.. Max-Planck-Institute for Solid State Research; Alemania Fil: Puphal, P.. Max-Planck-Institute for Solid State Research; Alemania Fil: Green, R. J.. University of British Columbia; Canadá. University of Saskatchewan; Canadá 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 Fil: Kim, J.. Argonne National Laboratory; Estados Unidos Fil: Casa, D.. Argonne National Laboratory; Estados Unidos Fil: Upton, M. H.. Argonne National Laboratory; Estados Unidos Fil: Wong, D.. Helmholtz-Zentrum Berlin für Materialien und Energie; Alemania Fil: Schulz, C.. Helmholtz-Zentrum Berlin für Materialien und Energie; Alemania Fil: Bartkowiak, M.. Helmholtz-Zentrum Berlin für Materialien und Energie; Alemania Fil: Habicht, K.. Universitat Potsdam; Alemania. Helmholtz-Zentrum Berlin für Materialien und Energie; Alemania Fil: Pomjakushina, E.. Paul Scherrer Institut; Suiza Fil: Cristiani, G.. Max Planck Institute For Solid State Research; Alemania Fil: Logvenov, G.. Max Planck Institute For Solid State Research; Alemania Fil: Minola, M.. Max Planck Institute For Solid State Research; Alemania Fil: Yamase, H.. Tsukuba University. National Institute For Materials Science; Japón 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 Fil: Keimer, B.. Max Planck Institute For Solid State Research; Alemania |
| description |
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. |
| publishDate |
2023 |
| dc.date.none.fl_str_mv |
2023-06 |
| dc.type.none.fl_str_mv |
info:eu-repo/semantics/article info:eu-repo/semantics/publishedVersion http://purl.org/coar/resource_type/c_6501 info:ar-repo/semantics/articulo |
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article |
| status_str |
publishedVersion |
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http://hdl.handle.net/11336/276609 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 2469-9950 2469-9969 CONICET Digital CONICET |
| url |
http://hdl.handle.net/11336/276609 |
| identifier_str_mv |
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 2469-9950 2469-9969 CONICET Digital CONICET |
| dc.language.none.fl_str_mv |
eng |
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eng |
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American Physical Society |
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American Physical Society |
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