Mottness at finite doping and charge instabilities in cuprates
The influence of Mott physics on the doping–temperature phase diagram of copper oxides represents a major issue that is the subject of intense theoretical and experimental efforts. Here, we investigate the ultrafast electron dynamics in prototypical single-layer Bi-based cuprates at the energy scale...
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Published in | Nature physics Vol. 13; no. 8; pp. 806 - 811 |
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Main Authors | , , , , , , , , , , , , , , |
Format | Journal Article |
Language | English |
Published |
London
Nature Publishing Group UK
01.08.2017
Nature Publishing Group |
Subjects | |
Online Access | Get full text |
ISSN | 1745-2473 1745-2481 |
DOI | 10.1038/nphys4112 |
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Abstract | The influence of Mott physics on the doping–temperature phase diagram of copper oxides represents a major issue that is the subject of intense theoretical and experimental efforts. Here, we investigate the ultrafast electron dynamics in prototypical single-layer Bi-based cuprates at the energy scale of the O-2
p
→ Cu-3
d
charge-transfer (CT) process. We demonstrate a clear evolution of the CT excitations from incoherent and localized, as in a Mott insulator, to coherent and delocalized, as in a conventional metal. This reorganization of the high-energy degrees of freedom occurs at the critical doping
p
cr
≈ 0.16 irrespective of the temperature, and it can be well described by dynamical mean-field theory calculations. We argue that the onset of low-temperature charge instabilities is the low-energy manifestation of the underlying Mottness that characterizes the
p
<
p
cr
region of the phase diagram. This discovery sets a new framework for theories of charge order and low-temperature phases in underdoped copper oxides.
The electron dynamics of single-layer Bi
2
Sr
2−
x
La
x
CuO
6+
δ
is studied as a function of doping, revealing the evolution of charge-transfer excitations from incoherent and localized (as in a Mott insulator) to coherent and delocalized (as in a conventional metal). |
---|---|
AbstractList | The influence of the Mott physics on the doping-temperature phase diagram of copper oxides represents a major issue that is subject of intense theoretical and experimental effort. Here, we investigate the ultrafast electron dynamics in prototypical single-layer Bi-based cuprates at the energy scale of the O-2p→Cu-3d charge-transfer (CT) process. We demonstrate a clear evolution of the CT excitations from incoherent and localized, as in a Mott insulator, to coherent and delocalized, as in a conventional metal. This reorganization of the high-energy degrees of freedom occurs at the critical doping pcr ≈0.16 irrespective of the temperature, and it can be well described by dynamical mean field theory calculations. We argue that the onset of the low-temperature charge instabilities is the low-energy manifestation of the underlying Mottness that characterizes the p < pcr region of the phase diagram. This discovery sets a new framework for theories of charge order and low-temperature phases in underdoped copper oxides.The influence of the Mott physics on the doping-temperature phase diagram of copper oxides represents a major issue that is subject of intense theoretical and experimental effort. Here, we investigate the ultrafast electron dynamics in prototypical single-layer Bi-based cuprates at the energy scale of the O-2p→Cu-3d charge-transfer (CT) process. We demonstrate a clear evolution of the CT excitations from incoherent and localized, as in a Mott insulator, to coherent and delocalized, as in a conventional metal. This reorganization of the high-energy degrees of freedom occurs at the critical doping pcr ≈0.16 irrespective of the temperature, and it can be well described by dynamical mean field theory calculations. We argue that the onset of the low-temperature charge instabilities is the low-energy manifestation of the underlying Mottness that characterizes the p < pcr region of the phase diagram. This discovery sets a new framework for theories of charge order and low-temperature phases in underdoped copper oxides. The influence of Mott physics on the doping–temperature phase diagram of copper oxides represents a major issue that is the subject of intense theoretical and experimental efforts. Here, we investigate the ultrafast electron dynamics in prototypical single-layer Bi-based cuprates at the energy scale of the O-2 p → Cu-3 d charge-transfer (CT) process. We demonstrate a clear evolution of the CT excitations from incoherent and localized, as in a Mott insulator, to coherent and delocalized, as in a conventional metal. This reorganization of the high-energy degrees of freedom occurs at the critical doping p cr ≈ 0.16 irrespective of the temperature, and it can be well described by dynamical mean-field theory calculations. We argue that the onset of low-temperature charge instabilities is the low-energy manifestation of the underlying Mottness that characterizes the p < p cr region of the phase diagram. This discovery sets a new framework for theories of charge order and low-temperature phases in underdoped copper oxides. The electron dynamics of single-layer Bi 2 Sr 2− x La x CuO 6+ δ is studied as a function of doping, revealing the evolution of charge-transfer excitations from incoherent and localized (as in a Mott insulator) to coherent and delocalized (as in a conventional metal). The influence of the Mott physics on the doping-temperature phase diagram of copper oxides represents a major issue that is subject of intense theoretical and experimental effort. Here, we investigate the ultrafast electron dynamics in prototypical single-layer Bi-based cuprates at the energy scale of the O-2 p →Cu-3 d charge-transfer (CT) process. We demonstrate a clear evolution of the CT excitations from incoherent and localized, as in a Mott insulator, to coherent and delocalized, as in a conventional metal. This reorganization of the high-energy degrees of freedom occurs at the critical doping p cr ≈0.16 irrespective of the temperature, and it can be well described by dynamical mean field theory calculations. We argue that the onset of the low-temperature charge instabilities is the low-energy manifestation of the underlying Mottness that characterizes the p < p cr region of the phase diagram. This discovery sets a new framework for theories of charge order and low-temperature phases in underdoped copper oxides. The influence of Mott physics on the doping-temperature phase diagram of copper oxides represents a major issue that is the subject of intense theoretical and experimental efforts. Here, we investigate the ultrafast electron dynamics in prototypical single-layer Bi-based cuprates at the energy scale of the O-2p -> Cu-3d charge-transfer (CT) process. We demonstrate a clear evolution of the CT excitations from incoherent and localized, as in a Mott insulator, to coherent and delocalized, as in a conventional metal. This reorganization of the high-energy degrees of freedom occurs at the critical doping pcr [ap] 0.16 irrespective of the temperature, and it can be well described by dynamical mean-field theory calculations. We argue that the onset of low-temperature charge instabilities is the low-energy manifestation of the underlying Mottness that characterizes the p < pcr region of the phase diagram. This discovery sets a new framework for theories of charge order and low-temperature phases in underdoped copper oxides. The influence of the Mott physics on the doping-temperature phase diagram of copper oxides represents a major issue that is subject of intense theoretical and experimental effort. Here, we investigate the ultrafast electron dynamics in prototypical single-layer Bi-based cuprates at the energy scale of the O-2 →Cu-3 charge-transfer (CT) process. We demonstrate a clear evolution of the CT excitations from incoherent and localized, as in a Mott insulator, to coherent and delocalized, as in a conventional metal. This reorganization of the high-energy degrees of freedom occurs at the critical doping ≈0.16 irrespective of the temperature, and it can be well described by dynamical mean field theory calculations. We argue that the onset of the low-temperature charge instabilities is the low-energy manifestation of the underlying Mottness that characterizes the < region of the phase diagram. This discovery sets a new framework for theories of charge order and low-temperature phases in underdoped copper oxides. |
Author | Banfi, F. Ferrini, G. Conte, S. Dal Ronchi, A. Damascelli, A. Abrami, P. Nembrini, N. Giannetti, C. Cerullo, G. Comin, R. Fabrizio, M. Peli, S. Brida, D. Lupi, S. Capone, M. |
AuthorAffiliation | 1 Department of Mathematics and Physics, Università Cattolica del Sacro Cuore, Brescia I-25121, Italy 7 Department of Physics and Astronomy, KU Leuven, Celestijnenlaan 200D, B-3001 Heverlee, Leuven, Belgium 10 Scuola Internazionale Superiore di Studi Avanzati (SISSA) and CNR-IOM Democritos National Simulation Center, Via Bonomea 265, 34136 Trieste (Italy) 3 IFN-CNR, Dipartimento di Fisica, Politecnico di Milano, 20133 Milano, Italy 8 Department of Physics and Center for Applied Photonics, University of Konstanz, 78457 Konstanz, Germany 9 CNR-IOM Dipartimento di Fisica, Università di Roma La Sapienza P.le Aldo Moro 2, 00185 Rome, Italy 2 Department of Physics, Università degli Studi di Milano, 20133 Milano, Italy 6 I-LAMP (Interdisciplinary Laboratories for Advanced Materials Physics), Università Cattolica del Sacro Cuore, Brescia I-25121, Italy 4 Quantum Matter Institute, University of British Columbia, Vancouver, BC V6T 1Z4, Canada 5 Department of Physics and Astronomy, University of British C |
AuthorAffiliation_xml | – name: 4 Quantum Matter Institute, University of British Columbia, Vancouver, BC V6T 1Z4, Canada – name: 5 Department of Physics and Astronomy, University of British Columbia, Vancouver, BC V6T 1Z1, Canada – name: 9 CNR-IOM Dipartimento di Fisica, Università di Roma La Sapienza P.le Aldo Moro 2, 00185 Rome, Italy – name: 1 Department of Mathematics and Physics, Università Cattolica del Sacro Cuore, Brescia I-25121, Italy – name: 8 Department of Physics and Center for Applied Photonics, University of Konstanz, 78457 Konstanz, Germany – name: 3 IFN-CNR, Dipartimento di Fisica, Politecnico di Milano, 20133 Milano, Italy – name: 10 Scuola Internazionale Superiore di Studi Avanzati (SISSA) and CNR-IOM Democritos National Simulation Center, Via Bonomea 265, 34136 Trieste (Italy) – name: 7 Department of Physics and Astronomy, KU Leuven, Celestijnenlaan 200D, B-3001 Heverlee, Leuven, Belgium – name: 2 Department of Physics, Università degli Studi di Milano, 20133 Milano, Italy – name: 6 I-LAMP (Interdisciplinary Laboratories for Advanced Materials Physics), Università Cattolica del Sacro Cuore, Brescia I-25121, Italy |
Author_xml | – sequence: 1 givenname: S. surname: Peli fullname: Peli, S. organization: Department of Mathematics and Physics, Università Cattolica del Sacro Cuore, Department of Physics, Università degli Studi di Milano – sequence: 2 givenname: S. Dal surname: Conte fullname: Conte, S. Dal organization: Dipartimento di Fisica, IFN-CNR, Politecnico di Milano – sequence: 3 givenname: R. surname: Comin fullname: Comin, R. organization: Quantum Matter Institute, University of British Columbia, Department of Physics and Astronomy, University of British Columbia, Present address: Department of Physics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139-4307, USA – sequence: 4 givenname: N. surname: Nembrini fullname: Nembrini, N. organization: Department of Mathematics and Physics, Università Cattolica del Sacro Cuore, Department of Physics, Università degli Studi di Milano – sequence: 5 givenname: A. surname: Ronchi fullname: Ronchi, A. organization: Department of Mathematics and Physics, Università Cattolica del Sacro Cuore, I-LAMP (Interdisciplinary Laboratories for Advanced Materials Physics), Università Cattolica del Sacro Cuore, Department of Physics and Astronomy – sequence: 6 givenname: P. surname: Abrami fullname: Abrami, P. organization: Department of Mathematics and Physics, Università Cattolica del Sacro Cuore, I-LAMP (Interdisciplinary Laboratories for Advanced Materials Physics), Università Cattolica del Sacro Cuore – sequence: 7 givenname: F. surname: Banfi fullname: Banfi, F. organization: Department of Mathematics and Physics, Università Cattolica del Sacro Cuore, I-LAMP (Interdisciplinary Laboratories for Advanced Materials Physics), Università Cattolica del Sacro Cuore – sequence: 8 givenname: G. surname: Ferrini fullname: Ferrini, G. organization: Department of Mathematics and Physics, Università Cattolica del Sacro Cuore, I-LAMP (Interdisciplinary Laboratories for Advanced Materials Physics), Università Cattolica del Sacro Cuore – sequence: 9 givenname: D. surname: Brida fullname: Brida, D. organization: Dipartimento di Fisica, IFN-CNR, Politecnico di Milano, Department of Physics and Center for Applied Photonics, University of Konstanz – sequence: 10 givenname: S. surname: Lupi fullname: Lupi, S. organization: CNR-IOM Dipartimento di Fisica, Università di Roma La Sapienza P.le Aldo Moro 2 – sequence: 11 givenname: M. surname: Fabrizio fullname: Fabrizio, M. organization: Scuola Internazionale Superiore di Studi Avanzati (SISSA) and CNR-IOM Democritos National Simulation Center – sequence: 12 givenname: A. surname: Damascelli fullname: Damascelli, A. organization: Quantum Matter Institute, University of British Columbia, Department of Physics and Astronomy, University of British Columbia – sequence: 13 givenname: M. surname: Capone fullname: Capone, M. organization: Scuola Internazionale Superiore di Studi Avanzati (SISSA) and CNR-IOM Democritos National Simulation Center – sequence: 14 givenname: G. surname: Cerullo fullname: Cerullo, G. organization: Dipartimento di Fisica, IFN-CNR, Politecnico di Milano – sequence: 15 givenname: C. surname: Giannetti fullname: Giannetti, C. email: claudio.giannetti@unicatt.it organization: Department of Mathematics and Physics, Università Cattolica del Sacro Cuore, I-LAMP (Interdisciplinary Laboratories for Advanced Materials Physics), Università Cattolica del Sacro Cuore |
BackLink | https://www.ncbi.nlm.nih.gov/pubmed/28781605$$D View this record in MEDLINE/PubMed |
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CitedBy_id | crossref_primary_10_1364_OE_514141 crossref_primary_10_1038_s41467_020_20824_7 crossref_primary_10_1103_PhysRevB_100_184302 crossref_primary_10_1103_PhysRevB_101_195128 crossref_primary_10_1103_PhysRevB_100_041116 crossref_primary_10_1038_s41598_024_56440_4 crossref_primary_10_1103_PhysRevB_110_115133 crossref_primary_10_1103_PhysRevLett_120_073201 crossref_primary_10_1126_sciadv_aar1998 crossref_primary_10_1038_s41567_024_02602_0 crossref_primary_10_1103_PhysRevB_106_054522 crossref_primary_10_1103_PhysRevB_109_014503 crossref_primary_10_1088_1361_6633_aaa97c crossref_primary_10_1103_PhysRevResearch_4_013101 crossref_primary_10_1103_PhysRevB_101_085127 crossref_primary_10_1016_j_xinn_2021_100202 crossref_primary_10_1103_PhysRevB_100_235117 crossref_primary_10_1103_PhysRevB_96_195141 crossref_primary_10_1103_PhysRevB_110_125102 |
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Snippet | The influence of Mott physics on the doping–temperature phase diagram of copper oxides represents a major issue that is the subject of intense theoretical and... The influence of the Mott physics on the doping-temperature phase diagram of copper oxides represents a major issue that is subject of intense theoretical and... The influence of Mott physics on the doping-temperature phase diagram of copper oxides represents a major issue that is the subject of intense theoretical and... |
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Title | Mottness at finite doping and charge instabilities in cuprates |
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