Pseudogaps: introducing the length scale into dynamical mean-field theory

Pseudogap physics in strongly correlated systems is essentially scale dependent. We generalize the dynamical mean-field theory (DMFT) by introducing into the DMFT equations dependence on the correlation length of pseudogap fluctuations via an additional (momentum-dependent) self-energy ∑k. Thi...

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Veröffentlicht in:Физика низких температур
Datum:2006
Hauptverfasser: Kuchinskii, E.Z., Nekrasov, I.A., Sadovskii, V.M.
Format: Artikel
Sprache:English
Veröffentlicht: Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України 2006
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Online Zugang:https://nasplib.isofts.kiev.ua/handle/123456789/120182
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Zitieren:Pseudogaps: introducing the length scale into dynamical mean-field theory / E.Z. Kuchinskii, I.A. Nekrasov, V.M. Sadovskii // Физика низких температур. — 2006. — Т. 32, № 4-5. — С. 528–537. — Бібліогр.: 23 назв. — англ.

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Digital Library of Periodicals of National Academy of Sciences of Ukraine
id nasplib_isofts_kiev_ua-123456789-120182
record_format dspace
spelling Kuchinskii, E.Z.
Nekrasov, I.A.
Sadovskii, V.M.
2017-06-11T12:00:20Z
2017-06-11T12:00:20Z
2006
Pseudogaps: introducing the length scale into dynamical mean-field theory / E.Z. Kuchinskii, I.A. Nekrasov, V.M. Sadovskii // Физика низких температур. — 2006. — Т. 32, № 4-5. — С. 528–537. — Бібліогр.: 23 назв. — англ.
0132-6414
PACS: 71.10.Fd, 71.10.Hf, 71.27.+a, 71.30.+h, 74.72.–h
https://nasplib.isofts.kiev.ua/handle/123456789/120182
Pseudogap physics in strongly correlated systems is essentially scale dependent. We generalize the dynamical mean-field theory (DMFT) by introducing into the DMFT equations dependence on the correlation length of pseudogap fluctuations via an additional (momentum-dependent) self-energy ∑k. This self-energy describes nonlocal dynamical correlations induced by short-ranged collective SDW-like antiferromagnetic spin (or CDW-like charge) fluctuations. At high enough temperatures these fluctuations can be viewed as a quenched Gaussian random field with finite correlation length. This generalized DMFT + ∑k approach is used for the numerical solution of the weakly doped one-band Hubbard model with repulsive Coulomb interaction on a square lattice with nearest and next nearest neighbor hopping. The effective single impurity problem is solved by the numerical renormalization group (NRG). Both types of strongly correlated metals, namely (i) the doped Mott insulator and (ii) the case of bandwidth W ≲ U (U is the value of local Coulomb interaction) are considered. Densities of states, spectral functions and ARPES spectra calculated within DMFT + ∑k show a pseudogap formation near the Fermi level of the quasiparticle band. We also briefly discuss effects of random impurity scattering. Finally we demonstrate the qualitative picture of Fermi surface «destruction» due to pseudogap fluctuations and formation of «Fermi arcs» which agrees well with ARPES observations.
We are grateful to Th. Pruschke for providing us with his NRG code and helpful discussions. This work was supported in part by RFBR grants 05-02-16301, 05-02-17244, and programs of the Presidium of the Russian Academy of Sciences (RAS) «Quantum macrophysics» and of the Division of Physical Sciences of the RAS «Strongly correlated electrons in semiconductors, metals, superconductors and magnetic materials». I.N. acknowledges support from the Dynasty Foundation and International Centre for Fundamental Physics in Moscow program for young scientists 2005 and Russian Science Support Foundation program for young PhD of the Russian Academy of Sciences 2005.
en
Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України
Физика низких температур
Pseudogap
Pseudogaps: introducing the length scale into dynamical mean-field theory
Article
published earlier
institution Digital Library of Periodicals of National Academy of Sciences of Ukraine
collection DSpace DC
title Pseudogaps: introducing the length scale into dynamical mean-field theory
spellingShingle Pseudogaps: introducing the length scale into dynamical mean-field theory
Kuchinskii, E.Z.
Nekrasov, I.A.
Sadovskii, V.M.
Pseudogap
title_short Pseudogaps: introducing the length scale into dynamical mean-field theory
title_full Pseudogaps: introducing the length scale into dynamical mean-field theory
title_fullStr Pseudogaps: introducing the length scale into dynamical mean-field theory
title_full_unstemmed Pseudogaps: introducing the length scale into dynamical mean-field theory
title_sort pseudogaps: introducing the length scale into dynamical mean-field theory
author Kuchinskii, E.Z.
Nekrasov, I.A.
Sadovskii, V.M.
author_facet Kuchinskii, E.Z.
Nekrasov, I.A.
Sadovskii, V.M.
topic Pseudogap
topic_facet Pseudogap
publishDate 2006
language English
container_title Физика низких температур
publisher Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України
format Article
description Pseudogap physics in strongly correlated systems is essentially scale dependent. We generalize the dynamical mean-field theory (DMFT) by introducing into the DMFT equations dependence on the correlation length of pseudogap fluctuations via an additional (momentum-dependent) self-energy ∑k. This self-energy describes nonlocal dynamical correlations induced by short-ranged collective SDW-like antiferromagnetic spin (or CDW-like charge) fluctuations. At high enough temperatures these fluctuations can be viewed as a quenched Gaussian random field with finite correlation length. This generalized DMFT + ∑k approach is used for the numerical solution of the weakly doped one-band Hubbard model with repulsive Coulomb interaction on a square lattice with nearest and next nearest neighbor hopping. The effective single impurity problem is solved by the numerical renormalization group (NRG). Both types of strongly correlated metals, namely (i) the doped Mott insulator and (ii) the case of bandwidth W ≲ U (U is the value of local Coulomb interaction) are considered. Densities of states, spectral functions and ARPES spectra calculated within DMFT + ∑k show a pseudogap formation near the Fermi level of the quasiparticle band. We also briefly discuss effects of random impurity scattering. Finally we demonstrate the qualitative picture of Fermi surface «destruction» due to pseudogap fluctuations and formation of «Fermi arcs» which agrees well with ARPES observations.
issn 0132-6414
url https://nasplib.isofts.kiev.ua/handle/123456789/120182
citation_txt Pseudogaps: introducing the length scale into dynamical mean-field theory / E.Z. Kuchinskii, I.A. Nekrasov, V.M. Sadovskii // Физика низких температур. — 2006. — Т. 32, № 4-5. — С. 528–537. — Бібліогр.: 23 назв. — англ.
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