Field theory of non-Hermitian disordered systems

The interplay between non-Hermiticity and disorder gives rise to unique universality classes of phase transitions and critical phenomena. Here, the authors develop effective field theory of non-Hermitian disordered systems and classify the universality classes across all the symmetry classes of non-Hermitian systems. The authors demonstrate that the phase transition characteristic of nonreciprocal disordered systems originates from the competition between kinetic and topological terms from the field-theoretical perspective.

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Publication Details

Journal
Physical review. B./Physical review. B
Published
2025-02-07
DOI
https://doi.org/10.1103/physrevb.111.054203
Citations
12
Primary Topic
Quantum Mechanics and Non-Hermitian Physics
Type
article
Field-Weighted Citation Impact
14.96

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article

Field theory of non-Hermitian disordered systems

Z. Y. Chen, Anish Kulkarni, Shinsei Ryu, Kohei Kawabata
12 citations
Physical review. B./Physical review. B
Quantum Mechanics and Non-Hermitian Physics
14.96
article

Field theory of non-Hermitian disordered systems

Z. Y. Chen, Anish Kulkarni, Shinsei Ryu, Kohei Kawabata
article en
12 citations

Abstract

The interplay between non-Hermiticity and disorder gives rise to unique universality classes of phase transitions and critical phenomena. Here, the authors develop effective field theory of non-Hermitian disordered systems and classify the universality classes across all the symmetry classes of non-Hermitian systems. The authors demonstrate that the phase transition characteristic of nonreciprocal disordered systems originates from the competition between kinetic and topological terms from the field-theoretical perspective.

Physical review. B./Physical review. BVol. 111(5)
Princeton University (US), The University of Tokyo (JP)
National Science Foundation, Gordon and Betty Moore Foundation, Japan Society for the Promotion of Science
Reduced inequalities
Openalex Percentile: Top 1%
Quantum Mechanics and Non-Hermitian Physics
14.96
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