Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Quantum phase transitions in the extended periodic Anderson model

昌久 古賀, Akihisa Koga

Published Jan 1, 2008• 0 citations
OpenAlex

Related papers

Quantum phase transitions in the bosonic single-impurity Anderson model

Jeong Yong Lee, R. Bulla

arXiv:cond-mat/0606325•The European Physical Journal B•Apr 1, 2007•13 citations

Phase diagram of the one dimensional periodic Anderson model

Raymond Chan, Ian P. McCulloch, M. Gulácsi

APS•Mar 1, 2004•0 citations

Quantum Criticality in the Two-Dimensional Periodic Anderson Model

Thomas Schäfer, A. A. Katanin, Motoharu Kitatani +2 more

Bulletin of the American Physical Society•Mar 8, 2019•0 citations

Quantum phase transitions in the extended periodic Anderson model

Akihisa Koga, Norio Kawakami, Robert Peters +1 more

We investigate quantum phase transitions in the extended periodic Anderson model, which includes electron correlations within and between itinerant and localized bands. We calculate zero and finite temperature properties of the system using the combination of dynamical mean-field theory and the numerical renormalization group. At half filling, a first-order phase transition between a Mott insulating state and a Kondo insulating state occurs in the strong-coupling regime. We furthermore find that a metallic state is stabilized in the weak-coupling regime. This state should be adiabatically connected to the orbital selective Mott state with one orbital-localized and the other itinerant. The effect of hole doping is also addressed.

arXiv:0708.1765•Physical Review B•Jan 15, 2008•24 citations

Quantum critical phase and Lifshitz transition in an extended periodic Anderson model

Laad, Mukul S., Koley, S., Taraphder, A.

We study the quantum phase transition in f -electron systems as a quantum Lifshitz transition driven by selective Mott localization in a realistic extended Anderson lattice model.Using DMFT, we find that a quantum critical phase with anomalous ω/T scaling separates a heavy Landau-Fermi liquid from ordered phase(s).Fermi surface reconstruction occurs via the interplay between, and penetration of the Green function zeros to the poles, leading to violation of Luttinger's theorem in the selective-Mott phase .We show how this naturally leads to scale-invariant responses in transport.Our work is represents a specific (DMFT) realization of the hidden-FL and FL * theories, and holds promise for study of "strange" metal phases in quantum matter.

•Jan 1, 2012•2 citations

Quantum Phase Transitions in Related Models

Amit Dutta, G. Aeppli, Bikas K. Chakrabarti +3 more

Cambridge University Press eBooks•Jan 28, 2015•0 citations
We investigate quantum phase transitions in the extended periodic Anderson model, which includes electron correlations within and between itinerant and localized bands. We calculate zero and finite temperature properties of the system using the combination of dynamical mean-field theory and the numerical renormalization group. At half filling, a first-order phase transition between a Mott insulating state and a Kondo insulating state occurs in the strong-coupling regime. We furthermore find that a metallic state is stabilized in the weak-coupling regime. This state should be adiabatically connected to the orbital selective Mott state with one orbital-localized and the other itinerant. The effect of hole doping is also addressed.
We study the quantum phase transition in f -electron systems as a quantum Lifshitz transition driven by selective Mott localization in a realistic extended Anderson lattice model.Using DMFT, we find that a quantum critical phase with anomalous ω/T scaling separates a heavy Landau-Fermi liquid from ordered phase(s).Fermi surface reconstruction occurs via the interplay between, and penetration of the Green function zeros to the poles, leading to violation of Luttinger's theorem in the selective-Mott phase .We show how this naturally leads to scale-invariant responses in transport.Our work is represents a specific (DMFT) realization of the hidden-FL and FL * theories, and holds promise for study of "strange" metal phases in quantum matter.