Non-fermi-liquid behavior in the periodic Anderson model
We study the Mott metal-insulator transition in the periodic Anderson model with dynamical mean field theory (DMFT). Near the quantum transition, we find a non-Fermi-liquid metallic state down to a vanishing temperature scale. We identify the origin of the non-Fermi-liquid behavior as being due to m...
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todo:paper_00319007_v101_n14_p_Amaricci2023-10-03T14:42:01Z Non-fermi-liquid behavior in the periodic Anderson model Amaricci, A. Sordi, G. Rozenberg, M.J. Fermi surface Fermions Magnetic anisotropy Magnetic fields Magnetic materials Magnetic properties Mean field theory Metal insulator boundaries Semiconductor insulator boundaries Semiconductor quantum dots Statistical mechanics Doped carriers Dynamical mean-field theory External magnetic fields Heavy fermion systems Localized moments Magnetic fluctuations Magnetic scattering Metal insulators Metallic states Non-Fermi-liquid Non-fermi-liquid behavior Periodic Anderson model Quantum transitions Metal insulator transition We study the Mott metal-insulator transition in the periodic Anderson model with dynamical mean field theory (DMFT). Near the quantum transition, we find a non-Fermi-liquid metallic state down to a vanishing temperature scale. We identify the origin of the non-Fermi-liquid behavior as being due to magnetic scattering of the doped carriers by the localized moments. The non-Fermi-liquid state can be tuned by either doping or external magnetic field. Our results show that the coupling to spatial magnetic fluctuations (absent in DMFT) is not a prerequisite to realizing a non-Fermi-liquid scenario for heavy fermion systems. © 2008 The American Physical Society. Fil:Rozenberg, M.J. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales; Argentina. JOUR info:eu-repo/semantics/openAccess http://creativecommons.org/licenses/by/2.5/ar http://hdl.handle.net/20.500.12110/paper_00319007_v101_n14_p_Amaricci |
institution |
Universidad de Buenos Aires |
institution_str |
I-28 |
repository_str |
R-134 |
collection |
Biblioteca Digital - Facultad de Ciencias Exactas y Naturales (UBA) |
topic |
Fermi surface Fermions Magnetic anisotropy Magnetic fields Magnetic materials Magnetic properties Mean field theory Metal insulator boundaries Semiconductor insulator boundaries Semiconductor quantum dots Statistical mechanics Doped carriers Dynamical mean-field theory External magnetic fields Heavy fermion systems Localized moments Magnetic fluctuations Magnetic scattering Metal insulators Metallic states Non-Fermi-liquid Non-fermi-liquid behavior Periodic Anderson model Quantum transitions Metal insulator transition |
spellingShingle |
Fermi surface Fermions Magnetic anisotropy Magnetic fields Magnetic materials Magnetic properties Mean field theory Metal insulator boundaries Semiconductor insulator boundaries Semiconductor quantum dots Statistical mechanics Doped carriers Dynamical mean-field theory External magnetic fields Heavy fermion systems Localized moments Magnetic fluctuations Magnetic scattering Metal insulators Metallic states Non-Fermi-liquid Non-fermi-liquid behavior Periodic Anderson model Quantum transitions Metal insulator transition Amaricci, A. Sordi, G. Rozenberg, M.J. Non-fermi-liquid behavior in the periodic Anderson model |
topic_facet |
Fermi surface Fermions Magnetic anisotropy Magnetic fields Magnetic materials Magnetic properties Mean field theory Metal insulator boundaries Semiconductor insulator boundaries Semiconductor quantum dots Statistical mechanics Doped carriers Dynamical mean-field theory External magnetic fields Heavy fermion systems Localized moments Magnetic fluctuations Magnetic scattering Metal insulators Metallic states Non-Fermi-liquid Non-fermi-liquid behavior Periodic Anderson model Quantum transitions Metal insulator transition |
description |
We study the Mott metal-insulator transition in the periodic Anderson model with dynamical mean field theory (DMFT). Near the quantum transition, we find a non-Fermi-liquid metallic state down to a vanishing temperature scale. We identify the origin of the non-Fermi-liquid behavior as being due to magnetic scattering of the doped carriers by the localized moments. The non-Fermi-liquid state can be tuned by either doping or external magnetic field. Our results show that the coupling to spatial magnetic fluctuations (absent in DMFT) is not a prerequisite to realizing a non-Fermi-liquid scenario for heavy fermion systems. © 2008 The American Physical Society. |
format |
JOUR |
author |
Amaricci, A. Sordi, G. Rozenberg, M.J. |
author_facet |
Amaricci, A. Sordi, G. Rozenberg, M.J. |
author_sort |
Amaricci, A. |
title |
Non-fermi-liquid behavior in the periodic Anderson model |
title_short |
Non-fermi-liquid behavior in the periodic Anderson model |
title_full |
Non-fermi-liquid behavior in the periodic Anderson model |
title_fullStr |
Non-fermi-liquid behavior in the periodic Anderson model |
title_full_unstemmed |
Non-fermi-liquid behavior in the periodic Anderson model |
title_sort |
non-fermi-liquid behavior in the periodic anderson model |
url |
http://hdl.handle.net/20.500.12110/paper_00319007_v101_n14_p_Amaricci |
work_keys_str_mv |
AT amariccia nonfermiliquidbehaviorintheperiodicandersonmodel AT sordig nonfermiliquidbehaviorintheperiodicandersonmodel AT rozenbergmj nonfermiliquidbehaviorintheperiodicandersonmodel |
_version_ |
1782026640985948160 |