Plasmon dispersion in bilayer cuprate superconductors
- Autores
- Bejas, Matias Hector; Zimmermann, V.; Betto, D.; Boyko, T. D.; Green, R. J.; Loew, T.; Brookes, N. B.; Cristiani, G.; Logvenov, G.; Minola, M.; Keimer, B.; Yamase, H.; Greco, Andres Francisco; Hepting, M.
- Año de publicación
- 2024
- Idioma
- inglés
- Tipo de recurso
- artículo
- Estado
- versión publicada
- Descripción
- The essential building blocks of cuprate superconductors are two-dimensional CuO2 sheets interspersed with charge reservoir layers. In bilayer cuprates, two closely spaced CuO2 sheets are separated by a larger distance from the subsequent pair in the next unit cell. In contrast to single-layer cuprates, prior theoretical work on bilayer systems has predicted two distinct acoustic plasmon bands for a given out-of-plane momentum transfer. Here we report random phase approximation (RPA) calculations for bilayer systems which corroborate the existence of two distinct plasmon bands. We find that the intensity of the lower-energy band is negligibly small in most parts of the Brillouin zone, whereas the higher-energy band carries significant spectral weight. We also present resonant inelastic x-ray scattering (RIXS) experiments at the O K-edge on the bilayer cuprate Y0.85Ca0.15Ba2Cu3O7 (Ca-YBCO), which show only one dispersive plasmon branch, in agreement with the RPA calculations. In addition, the RPA results indicate that the dispersion of the higher-energy plasmon band in Ca-YBCO is not strictly acoustic but exhibits a substantial energy gap of approximately 250 meV at the two-dimensional Brillouin zone center.
Fil: Bejas, Matias Hector. Universidad Nacional de Rosario. Facultad de Ciencias Exactas, Ingeniería y Agrimensura; Argentina. 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: Zimmermann, V.. Max Planck Institute For Solid State Research; Alemania
Fil: Betto, D.. No especifíca;
Fil: Boyko, T. D.. No especifíca;
Fil: Green, R. J.. University of British Columbia; Canadá. University of Saskatchewan; Canadá
Fil: Loew, T.. Max Planck Institute For Solid State Research; Alemania
Fil: Brookes, N. B.. No especifíca;
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: Keimer, B.. Max Planck Institute For Solid State Research; Alemania
Fil: Yamase, H.. 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. Universidad Nacional de Rosario. Facultad de Ciencias Exactas, Ingeniería y Agrimensura; Argentina
Fil: Hepting, M.. Max Planck Institute For Solid State Research; Alemania - Materia
-
SUPERCONDUCTIVITY
UNCONVENTIONAL SUPERCONDUCTORS
X-RAY TECHNIQUES - Nivel de accesibilidad
- acceso abierto
- Condiciones de uso
- https://creativecommons.org/licenses/by-nc-sa/2.5/ar/
- Repositorio
- Institución
- Consejo Nacional de Investigaciones Científicas y Técnicas
- OAI Identificador
- oai:ri.conicet.gov.ar:11336/267320
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Plasmon dispersion in bilayer cuprate superconductorsBejas, Matias HectorZimmermann, V.Betto, D.Boyko, T. D.Green, R. J.Loew, T.Brookes, N. B.Cristiani, G.Logvenov, G.Minola, M.Keimer, B.Yamase, H.Greco, Andres FranciscoHepting, M.SUPERCONDUCTIVITYUNCONVENTIONAL SUPERCONDUCTORSX-RAY TECHNIQUEShttps://purl.org/becyt/ford/1.3https://purl.org/becyt/ford/1The essential building blocks of cuprate superconductors are two-dimensional CuO2 sheets interspersed with charge reservoir layers. In bilayer cuprates, two closely spaced CuO2 sheets are separated by a larger distance from the subsequent pair in the next unit cell. In contrast to single-layer cuprates, prior theoretical work on bilayer systems has predicted two distinct acoustic plasmon bands for a given out-of-plane momentum transfer. Here we report random phase approximation (RPA) calculations for bilayer systems which corroborate the existence of two distinct plasmon bands. We find that the intensity of the lower-energy band is negligibly small in most parts of the Brillouin zone, whereas the higher-energy band carries significant spectral weight. We also present resonant inelastic x-ray scattering (RIXS) experiments at the O K-edge on the bilayer cuprate Y0.85Ca0.15Ba2Cu3O7 (Ca-YBCO), which show only one dispersive plasmon branch, in agreement with the RPA calculations. In addition, the RPA results indicate that the dispersion of the higher-energy plasmon band in Ca-YBCO is not strictly acoustic but exhibits a substantial energy gap of approximately 250 meV at the two-dimensional Brillouin zone center.Fil: Bejas, Matias Hector. Universidad Nacional de Rosario. Facultad de Ciencias Exactas, Ingeniería y Agrimensura; Argentina. 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: Zimmermann, V.. Max Planck Institute For Solid State Research; AlemaniaFil: Betto, D.. No especifíca;Fil: Boyko, T. D.. No especifíca;Fil: Green, R. J.. University of British Columbia; Canadá. University of Saskatchewan; CanadáFil: Loew, T.. Max Planck Institute For Solid State Research; AlemaniaFil: Brookes, N. B.. No especifíca;Fil: 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: Keimer, B.. Max Planck Institute For Solid State Research; AlemaniaFil: Yamase, H.. 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; Argentina. Universidad Nacional de Rosario. Facultad de Ciencias Exactas, Ingeniería y Agrimensura; ArgentinaFil: Hepting, M.. Max Planck Institute For Solid State Research; AlemaniaAmerican Physical Society2024-04info:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersionhttp://purl.org/coar/resource_type/c_6501info:ar-repo/semantics/articuloapplication/pdfapplication/pdfapplication/pdfhttp://hdl.handle.net/11336/267320Bejas, Matias Hector; Zimmermann, V.; Betto, D.; Boyko, T. D.; Green, R. J.; et al.; Plasmon dispersion in bilayer cuprate superconductors; American Physical Society; Physical Review B; 109; 14; 4-2024; 1-92469-99502469-9969CONICET DigitalCONICETenginfo:eu-repo/semantics/altIdentifier/url/https://link.aps.org/doi/10.1103/PhysRevB.109.144516info:eu-repo/semantics/altIdentifier/doi/10.1103/PhysRevB.109.144516info:eu-repo/semantics/openAccesshttps://creativecommons.org/licenses/by-nc-sa/2.5/ar/reponame:CONICET Digital (CONICET)instname:Consejo Nacional de Investigaciones Científicas y Técnicas2025-09-29T09:58:26Zoai:ri.conicet.gov.ar:11336/267320instacron: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:34982025-09-29 09:58:26.442CONICET Digital (CONICET) - Consejo Nacional de Investigaciones Científicas y Técnicasfalse |
dc.title.none.fl_str_mv |
Plasmon dispersion in bilayer cuprate superconductors |
title |
Plasmon dispersion in bilayer cuprate superconductors |
spellingShingle |
Plasmon dispersion in bilayer cuprate superconductors Bejas, Matias Hector SUPERCONDUCTIVITY UNCONVENTIONAL SUPERCONDUCTORS X-RAY TECHNIQUES |
title_short |
Plasmon dispersion in bilayer cuprate superconductors |
title_full |
Plasmon dispersion in bilayer cuprate superconductors |
title_fullStr |
Plasmon dispersion in bilayer cuprate superconductors |
title_full_unstemmed |
Plasmon dispersion in bilayer cuprate superconductors |
title_sort |
Plasmon dispersion in bilayer cuprate superconductors |
dc.creator.none.fl_str_mv |
Bejas, Matias Hector Zimmermann, V. Betto, D. Boyko, T. D. Green, R. J. Loew, T. Brookes, N. B. Cristiani, G. Logvenov, G. Minola, M. Keimer, B. Yamase, H. Greco, Andres Francisco Hepting, M. |
author |
Bejas, Matias Hector |
author_facet |
Bejas, Matias Hector Zimmermann, V. Betto, D. Boyko, T. D. Green, R. J. Loew, T. Brookes, N. B. Cristiani, G. Logvenov, G. Minola, M. Keimer, B. Yamase, H. Greco, Andres Francisco Hepting, M. |
author_role |
author |
author2 |
Zimmermann, V. Betto, D. Boyko, T. D. Green, R. J. Loew, T. Brookes, N. B. Cristiani, G. Logvenov, G. Minola, M. Keimer, B. Yamase, H. Greco, Andres Francisco Hepting, M. |
author2_role |
author author author author author author author author author author author author author |
dc.subject.none.fl_str_mv |
SUPERCONDUCTIVITY UNCONVENTIONAL SUPERCONDUCTORS X-RAY TECHNIQUES |
topic |
SUPERCONDUCTIVITY UNCONVENTIONAL SUPERCONDUCTORS X-RAY TECHNIQUES |
purl_subject.fl_str_mv |
https://purl.org/becyt/ford/1.3 https://purl.org/becyt/ford/1 |
dc.description.none.fl_txt_mv |
The essential building blocks of cuprate superconductors are two-dimensional CuO2 sheets interspersed with charge reservoir layers. In bilayer cuprates, two closely spaced CuO2 sheets are separated by a larger distance from the subsequent pair in the next unit cell. In contrast to single-layer cuprates, prior theoretical work on bilayer systems has predicted two distinct acoustic plasmon bands for a given out-of-plane momentum transfer. Here we report random phase approximation (RPA) calculations for bilayer systems which corroborate the existence of two distinct plasmon bands. We find that the intensity of the lower-energy band is negligibly small in most parts of the Brillouin zone, whereas the higher-energy band carries significant spectral weight. We also present resonant inelastic x-ray scattering (RIXS) experiments at the O K-edge on the bilayer cuprate Y0.85Ca0.15Ba2Cu3O7 (Ca-YBCO), which show only one dispersive plasmon branch, in agreement with the RPA calculations. In addition, the RPA results indicate that the dispersion of the higher-energy plasmon band in Ca-YBCO is not strictly acoustic but exhibits a substantial energy gap of approximately 250 meV at the two-dimensional Brillouin zone center. Fil: Bejas, Matias Hector. Universidad Nacional de Rosario. Facultad de Ciencias Exactas, Ingeniería y Agrimensura; Argentina. 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: Zimmermann, V.. Max Planck Institute For Solid State Research; Alemania Fil: Betto, D.. No especifíca; Fil: Boyko, T. D.. No especifíca; Fil: Green, R. J.. University of British Columbia; Canadá. University of Saskatchewan; Canadá Fil: Loew, T.. Max Planck Institute For Solid State Research; Alemania Fil: Brookes, N. B.. No especifíca; 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: Keimer, B.. Max Planck Institute For Solid State Research; Alemania Fil: Yamase, H.. 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. Universidad Nacional de Rosario. Facultad de Ciencias Exactas, Ingeniería y Agrimensura; Argentina Fil: Hepting, M.. Max Planck Institute For Solid State Research; Alemania |
description |
The essential building blocks of cuprate superconductors are two-dimensional CuO2 sheets interspersed with charge reservoir layers. In bilayer cuprates, two closely spaced CuO2 sheets are separated by a larger distance from the subsequent pair in the next unit cell. In contrast to single-layer cuprates, prior theoretical work on bilayer systems has predicted two distinct acoustic plasmon bands for a given out-of-plane momentum transfer. Here we report random phase approximation (RPA) calculations for bilayer systems which corroborate the existence of two distinct plasmon bands. We find that the intensity of the lower-energy band is negligibly small in most parts of the Brillouin zone, whereas the higher-energy band carries significant spectral weight. We also present resonant inelastic x-ray scattering (RIXS) experiments at the O K-edge on the bilayer cuprate Y0.85Ca0.15Ba2Cu3O7 (Ca-YBCO), which show only one dispersive plasmon branch, in agreement with the RPA calculations. In addition, the RPA results indicate that the dispersion of the higher-energy plasmon band in Ca-YBCO is not strictly acoustic but exhibits a substantial energy gap of approximately 250 meV at the two-dimensional Brillouin zone center. |
publishDate |
2024 |
dc.date.none.fl_str_mv |
2024-04 |
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 |
format |
article |
status_str |
publishedVersion |
dc.identifier.none.fl_str_mv |
http://hdl.handle.net/11336/267320 Bejas, Matias Hector; Zimmermann, V.; Betto, D.; Boyko, T. D.; Green, R. J.; et al.; Plasmon dispersion in bilayer cuprate superconductors; American Physical Society; Physical Review B; 109; 14; 4-2024; 1-9 2469-9950 2469-9969 CONICET Digital CONICET |
url |
http://hdl.handle.net/11336/267320 |
identifier_str_mv |
Bejas, Matias Hector; Zimmermann, V.; Betto, D.; Boyko, T. D.; Green, R. J.; et al.; Plasmon dispersion in bilayer cuprate superconductors; American Physical Society; Physical Review B; 109; 14; 4-2024; 1-9 2469-9950 2469-9969 CONICET Digital CONICET |
dc.language.none.fl_str_mv |
eng |
language |
eng |
dc.relation.none.fl_str_mv |
info:eu-repo/semantics/altIdentifier/url/https://link.aps.org/doi/10.1103/PhysRevB.109.144516 info:eu-repo/semantics/altIdentifier/doi/10.1103/PhysRevB.109.144516 |
dc.rights.none.fl_str_mv |
info:eu-repo/semantics/openAccess https://creativecommons.org/licenses/by-nc-sa/2.5/ar/ |
eu_rights_str_mv |
openAccess |
rights_invalid_str_mv |
https://creativecommons.org/licenses/by-nc-sa/2.5/ar/ |
dc.format.none.fl_str_mv |
application/pdf application/pdf application/pdf |
dc.publisher.none.fl_str_mv |
American Physical Society |
publisher.none.fl_str_mv |
American Physical Society |
dc.source.none.fl_str_mv |
reponame:CONICET Digital (CONICET) instname:Consejo Nacional de Investigaciones Científicas y Técnicas |
reponame_str |
CONICET Digital (CONICET) |
collection |
CONICET Digital (CONICET) |
instname_str |
Consejo Nacional de Investigaciones Científicas y Técnicas |
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CONICET Digital (CONICET) - Consejo Nacional de Investigaciones Científicas y Técnicas |
repository.mail.fl_str_mv |
dasensio@conicet.gov.ar; lcarlino@conicet.gov.ar |
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1844613741219414016 |
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13.070432 |