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Electron Glass Phase with Resilient Zhang-Rice Singlets in LiCu_{3}O_{3}.
Consiglio, A; Gatti, G; Martino, E; Moreschini, L; Johannsen, J C; Prsa, K; Freeman, P G; Sheptyakov, D; Rønnow, H M; Scopelliti, R; Magrez, A; Forró, L; Schmitt, C; Jovic, V; Jozwiak, C; Bostwick, A; Rotenberg, E; Hofmann, T; Thomale, R; Sangiovanni, G; Di Sante, D; Greiter, M; Grioni, M; Moser, S.
Affiliation
  • Consiglio A; Institut für Theoretische Physik und Astrophysik and Würzburg-Dresden Cluster of Excellence ct.qmat, Universität Würzburg, 97074 Würzburg, Germany.
  • Gatti G; Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), CH-1015 Lausanne, Switzerland.
  • Martino E; Department of Quantum Matter Physics, University of Geneva, 24 Quai Ernest-Ansermet, 1211 Geneva, Switzerland.
  • Moreschini L; Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), CH-1015 Lausanne, Switzerland.
  • Johannsen JC; Advanced Light Source (ALS), Berkeley, California 94720, USA.
  • Prsa K; Materials Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA.
  • Freeman PG; Department of Physics, University of California, Berkeley, Berkeley, California 94720, USA.
  • Sheptyakov D; Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), CH-1015 Lausanne, Switzerland.
  • Rønnow HM; Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), CH-1015 Lausanne, Switzerland.
  • Scopelliti R; Laboratory for Neutron Scattering and Imaging, Paul Scherrer Institut, 5232 Villigen PSI, Switzerland.
  • Magrez A; Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), CH-1015 Lausanne, Switzerland.
  • Forró L; Jeremiah Horrocks Institute for Mathematics, Physics and Astronomy, University of Central Lancashire, Preston PR1 2HE, United Kingdom.
  • Schmitt C; Laboratory for Neutron Scattering and Imaging, Paul Scherrer Institut, 5232 Villigen PSI, Switzerland.
  • Jovic V; Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), CH-1015 Lausanne, Switzerland.
  • Jozwiak C; Institute of Chemical Sciences and Engineering, Ecole Polytechnique Fédérale de Lausanne (EPFL), CH-1015 Lausanne, Switzerland.
  • Bostwick A; Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), CH-1015 Lausanne, Switzerland.
  • Rotenberg E; Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), CH-1015 Lausanne, Switzerland.
  • Hofmann T; Stavropoulos Center for Complex Quantum Matter, Department of Physics and Astronomy, University of Notre Dame, Notre Dame, Indiana 46556, USA.
  • Thomale R; Physikalisches Institut and Würzburg-Dresden Cluster of Excellence ct.qmat, Universität Würzburg, Würzburg 97074, Germany.
  • Sangiovanni G; Advanced Light Source (ALS), Berkeley, California 94720, USA.
  • Di Sante D; Earth Resources and Materials, Institute of Geological and Nuclear Science, Lower Hutt 5010, New Zealand and MacDiarmid Institute for Advanced Materials and Nanotechnology, Wellington 6012, New Zealand.
  • Greiter M; Advanced Light Source (ALS), Berkeley, California 94720, USA.
  • Grioni M; Advanced Light Source (ALS), Berkeley, California 94720, USA.
  • Moser S; Advanced Light Source (ALS), Berkeley, California 94720, USA.
Phys Rev Lett ; 132(12): 126502, 2024 Mar 22.
Article in En | MEDLINE | ID: mdl-38579201
ABSTRACT
LiCu_{3}O_{3} is an antiferromagnetic mixed valence cuprate where trilayers of edge-sharing Cu(II)O (3d^{9}) are sandwiched in between planes of Cu(I) (3d^{10}) ions, with Li stochastically substituting Cu(II). Angle-resolved photoemission spectroscopy (ARPES) and density functional theory reveal two insulating electronic subsystems that are segregated in spite of sharing common oxygen atoms a Cu d_{z^{2}}/O p_{z} derived valence band (VB) dispersing on the Cu(I) plane, and a Cu 3d_{x^{2}-y^{2}}/O 2p_{x,y} derived Zhang-Rice singlet (ZRS) band dispersing on the Cu(II)O planes. First-principle analysis shows the Li substitution to stabilize the insulating ground state, but only if antiferromagnetic correlations are present. Li further induces substitutional disorder and a 2D electron glass behavior in charge transport, reflected in a large 530 meV Coulomb gap and a linear suppression of VB spectral weight at E_{F} that is observed by ARPES. Surprisingly, the disorder leaves the Cu(II)-derived ZRS largely unaffected. This indicates a local segregation of Li and Cu atoms onto the two separate corner-sharing Cu(II)O_{2} sub-lattices of the edge-sharing Cu(II)O planes, and highlights the ubiquitous resilience of the entangled two hole ZRS entity against impurity scattering.

Full text: 1 Collection: 01-internacional Database: MEDLINE Language: En Journal: Phys Rev Lett / Phys. rev. lett / Physical review letters Year: 2024 Type: Article Affiliation country: Germany

Full text: 1 Collection: 01-internacional Database: MEDLINE Language: En Journal: Phys Rev Lett / Phys. rev. lett / Physical review letters Year: 2024 Type: Article Affiliation country: Germany