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

APS

Multi-Channel Kondo Effect in an Interacting Electron System

Mats Granath, Henrik Johannesson

Published Mar 1, 1997• 0 citations
OpenAlex

Related papers

Destruction of the Kondo effect in a multi-channel Bose–Fermi Kondo model

Stefan Kirchner, Lijun Zhu, Qimiao Si A

arXiv:cond-mat/0407307•Physica B Condensed Matter•Feb 15, 2005•3 citations

Observation of the Multi-channel ‘charge’ Kondo Effect

Zubair Iftikhar

Springer theses•Jan 1, 2018•0 citations

Kondo effect in a one dimensional interacting electron system

H.-U. Desgranges

Springer eBooks•Apr 6, 2008•0 citations

Quantum Phase Transition in Multi-channel Kondo Systems

Zubair Iftikhar

Springer theses•Jan 1, 2018•1 citation

Exact results on the multi-channel Kondo effect from conformal field theory

Andreas W. W. Ludwig

Physica B Condensed Matter•Apr 1, 1994•10 citations

Probing Collective and Individual Kondo Screening: Multi-Stage, Multi-Channel Kondo Effects in a $C_3$-Symmetric Four-Impurity Model

Danqing Hu, Jiangfan Wang, Zixiang Hu +1 more

Collective screening has been proposed to underlie the basic physics of multi-impurity and lattice Kondo systems. But how to establish this picture and distinguish it from individual (local) Kondo screening remains a grand challenge. The recently developed auxiliary-bath numerical renormalization group (AUNRG) method provides a key step towards resolving this issue. Its application to the $C_3$-symmetric three-impurity Kondo (3IK) model with a shared electron bath reveals fully screened Fermi liquid ground states arising from collective screening of cluster spin degrees of freedom at small Kondo coupling $J_{\rm K}$ and individual (local) screening of local impurities at large $J_{\rm K}$. Here we design a four-impurity Kondo (4IK) model where the probe impurity couples only to the original three Kondo impurities to detect the nature of the screened states. We show that the collective and individual Kondo screenings give rise to emergent multi-stage, two-channel Kondo effect and unstable three-channel Kondo effect, respectively. This suggests a special helicity structure of the screened states and confirms the idea of collective screening in multi-impurity Kondo systems. Our work also demonstrates that the same auxiliary-bath construction can be readily extended to models with additional impurities to explore novel many-body quantum states with emergent cluster degrees of freedom.

arXiv:2609.40109•Sep 30, 2026•0 citations
Probing Collective and Individual Kondo Screening: Multi-Stage, Multi-Channel Kondo Effects in a C3C_3C3​-Symmetric Four-Impurity Model
Collective screening has been proposed to underlie the basic physics of multi-impurity and lattice Kondo systems. But how to establish this picture and distinguish it from individual (local) Kondo screening remains a grand challenge. The recently developed auxiliary-bath numerical renormalization group (AUNRG) method provides a key step towards resolving this issue. Its application to the C3C_3C3​-symmetric three-impurity Kondo (3IK) model with a shared electron bath reveals fully screened Fermi liquid ground states arising from collective screening of cluster spin degrees of freedom at small Kondo coupling JKJ_{\rm K}JK​ and individual (local) screening of local impurities at large JKJ_{\rm K}JK​. Here we design a four-impurity Kondo (4IK) model where the probe impurity couples only to the original three Kondo impurities to detect the nature of the screened states. We show that the collective and individual Kondo screenings give rise to emergent multi-stage, two-channel Kondo effect and unstable three-channel Kondo effect, respectively. This suggests a special helicity structure of the screened states and confirms the idea of collective screening in multi-impurity Kondo systems. Our work also demonstrates that the same auxiliary-bath construction can be readily extended to models with additional impurities to explore novel many-body quantum states with emergent cluster degrees of freedom.