Fermionic quantum criticality through the lens of topological holography

We utilize the topological holographic framework to characterize and gain insights into the nature of quantum critical points and gapless phases in fermionic quantum systems. Topological holography is a general framework that describes the generalized global symmetry and the symmetry charges of a local quantum system in terms of a slab of a topological order, termed as the symmetry topological field theory (SymTFT), in one higher dimension. In this work, we consider a generalization of the topological holographic picture for (1+1)<a:math xmlns:a="http://www.w3.org/1998/Math/MathML"><a:mi>d</a:mi></a:math> fermionic quantum phases of matter. We discuss how spin structures are encoded in the SymTFT, and we establish the connection between the formal fermionization formula in quantum field theory and the choice of fermionic gapped boundary conditions of the SymTFT. We demonstrate the identification and the characterization of the fermionic gapped phases and phase transitions through detailed analysis of various examples, including the fermionic systems with <b:math xmlns:b="http://www.w3.org/1998/Math/MathML"><b:msubsup><b:mi mathvariant="double-struck">Z</b:mi><b:mn>2</b:mn><b:mi>F</b:mi></b:msubsup><b:mo>,</b:mo><b:mo> </b:mo><b:mrow><b:msub><b:mi mathvariant="double-struck">Z</b:mi><b:mn>2</b:mn></b:msub><b:mo>×</b:mo><b:msubsup><b:mi mathvariant="double-struck">Z</b:mi><b:mn>2</b:mn><b:mi>F</b:mi></b:msubsup></b:mrow><b:mo>,</b:mo><b:mo> </b:mo><b:msubsup><b:mi mathvariant="double-struck">Z</b:mi><b:mrow><b:mn>4</b:mn></b:mrow><b:mi>F</b:mi></b:msubsup></b:math>, and the fermionic version of the noninvertible <g:math xmlns:g="http://www.w3.org/1998/Math/MathML"><g:mrow><g:mtext>Rep</g:mtext><g:mo>(</g:mo><g:msub><g:mi>S</g:mi><g:mn>3</g:mn></g:msub><g:mo>)</g:mo></g:mrow></g:math> symmetry. Our work uncovers many exotic fermionic gapped phases, quantum critical points, and gapless phases. These include gapped phases with fermionic noninvertible <h:math xmlns:h="http://www.w3.org/1998/Math/MathML"><h:mrow><h:mtext>Rep</h:mtext><h:mo>(</h:mo><h:msub><h:mi>S</h:mi><h:mn>3</h:mn></h:msub><h:mo>)</h:mo></h:mrow></h:math> symmetry, two kinds of fermionic symmetry-enriched quantum critical points, a fermionic gapless symmetry-protected topological phase, and a fermionic gapless spontaneous symmetry-breaking phase that breaks the fermionic noninvertible symmetry.

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Publication Details

Journal
Physical review. B./Physical review. B
Published
2025-04-18
DOI
https://doi.org/10.1103/physrevb.111.155130
Citations
10
Primary Topic
Topological Materials and Phenomena
Type
article
Field-Weighted Citation Impact
12.47
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article

Fermionic quantum criticality through the lens of topological holography

Sheng-Jie Huang
10 citations
Physical review. B./Physical review. B
Topological Materials and Phenomena
12.47
article

Fermionic quantum criticality through the lens of topological holography

Sheng-Jie Huang
article en
10 citations

Abstract

We utilize the topological holographic framework to characterize and gain insights into the nature of quantum critical points and gapless phases in fermionic quantum systems. Topological holography is a general framework that describes the generalized global symmetry and the symmetry charges of a local quantum system in terms of a slab of a topological order, termed as the symmetry topological field theory (SymTFT), in one higher dimension. In this work, we consider a generalization of the topological holographic picture for (1+1)<a:math xmlns:a="http://www.w3.org/1998/Math/MathML"><a:mi>d</a:mi></a:math> fermionic quantum phases of matter. We discuss how spin structures are encoded in the SymTFT, and we establish the connection between the formal fermionization formula in quantum field theory and the choice of fermionic gapped boundary conditions of the SymTFT. We demonstrate the identification and the characterization of the fermionic gapped phases and phase transitions through detailed analysis of various examples, including the fermionic systems with <b:math xmlns:b="http://www.w3.org/1998/Math/MathML"><b:msubsup><b:mi mathvariant="double-struck">Z</b:mi><b:mn>2</b:mn><b:mi>F</b:mi></b:msubsup><b:mo>,</b:mo><b:mo> </b:mo><b:mrow><b:msub><b:mi mathvariant="double-struck">Z</b:mi><b:mn>2</b:mn></b:msub><b:mo>×</b:mo><b:msubsup><b:mi mathvariant="double-struck">Z</b:mi><b:mn>2</b:mn><b:mi>F</b:mi></b:msubsup></b:mrow><b:mo>,</b:mo><b:mo> </b:mo><b:msubsup><b:mi mathvariant="double-struck">Z</b:mi><b:mrow><b:mn>4</b:mn></b:mrow><b:mi>F</b:mi></b:msubsup></b:math>, and the fermionic version of the noninvertible <g:math xmlns:g="http://www.w3.org/1998/Math/MathML"><g:mrow><g:mtext>Rep</g:mtext><g:mo>(</g:mo><g:msub><g:mi>S</g:mi><g:mn>3</g:mn></g:msub><g:mo>)</g:mo></g:mrow></g:math> symmetry. Our work uncovers many exotic fermionic gapped phases, quantum critical points, and gapless phases. These include gapped phases with fermionic noninvertible <h:math xmlns:h="http://www.w3.org/1998/Math/MathML"><h:mrow><h:mtext>Rep</h:mtext><h:mo>(</h:mo><h:msub><h:mi>S</h:mi><h:mn>3</h:mn></h:msub><h:mo>)</h:mo></h:mrow></h:math> symmetry, two kinds of fermionic symmetry-enriched quantum critical points, a fermionic gapless symmetry-protected topological phase, and a fermionic gapless spontaneous symmetry-breaking phase that breaks the fermionic noninvertible symmetry.

Physical review. B./Physical review. BVol. 111(15)
Max Planck Institute for the Physics of Complex Systems (DE)
Openalex Percentile: Top 1%
Topological Materials and Phenomena
12.47
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