Quantum chaos from multiple copies of integrable commuting SYK models

We construct a new family of quantum chaotic models by combining multiple copies of integrable commuting SYK models. As each copy of the commuting SYK model does not commute with others, this construction breaks the integrability of each commuting SYK and the family of models demonstrates the emergence of quantum chaos. We study the spectrum of this model analytically in the double-scaled limit. As the number of copies tends to infinity, the spectrum becomes compact and equivalent to the regular SYK model. For finite <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"><a:mi>d</a:mi></a:math> copies, the spectrum is close to the regular SYK model in UV but has an exponential tail <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"><c:msup><c:mi>e</c:mi><c:mrow><c:mi>E</c:mi><c:mo>/</c:mo><c:msub><c:mi>T</c:mi><c:mi>c</c:mi></c:msub></c:mrow></c:msup></c:math> in the IR. We identify the reciprocal of the exponent in the tail as a critical temperature <e:math xmlns:e="http://www.w3.org/1998/Math/MathML" display="inline"><e:msub><e:mi>T</e:mi><e:mi>c</e:mi></e:msub></e:math>, above which the model should be quantum chaotic. <g:math xmlns:g="http://www.w3.org/1998/Math/MathML" display="inline"><g:msub><g:mi>T</g:mi><g:mi>c</g:mi></g:msub></g:math> monotonically decreases as <i:math xmlns:i="http://www.w3.org/1998/Math/MathML" display="inline"><i:mi>d</i:mi></i:math> increases, which expands the chaotic regime over the nonchaotic regime. We propose the existence of a new phase around <k:math xmlns:k="http://www.w3.org/1998/Math/MathML" display="inline"><k:msub><k:mi>T</k:mi><k:mi>c</k:mi></k:msub></k:math>, and the dynamics should be very different in two phases. We further carry out numeric analysis at finite <m:math xmlns:m="http://www.w3.org/1998/Math/MathML" display="inline"><m:mi>d</m:mi></m:math>, which supports our proposal. Given any finite dimensional local Hamiltonian, by decomposing it into <o:math xmlns:o="http://www.w3.org/1998/Math/MathML" display="inline"><o:mi>d</o:mi></o:math> groups, in which all terms in one group commute with each other but terms from different groups may not, our analysis can give an estimate of the critical temperature for quantum chaos based on the decomposition. We also comment on the implication of the critical temperature to future quantum simulations of quantum chaos and quantum gravity.

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Journal
Physical review. D/Physical review. D.
Published
2025-07-19
DOI
https://doi.org/10.1103/1k6k-xhmk
Citations
3
Primary Topic
Nonlinear Waves and Solitons
Type
article
Field-Weighted Citation Impact
3.97
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article

Quantum chaos from multiple copies of integrable commuting SYK models

Karl J. Friston
3 citations
Physical review. D/Physical review. D.
Nonlinear Waves and Solitons
3.97
article

Quantum chaos from multiple copies of integrable commuting SYK models

Karl J. Friston
article en
3 citations

Abstract

We construct a new family of quantum chaotic models by combining multiple copies of integrable commuting SYK models. As each copy of the commuting SYK model does not commute with others, this construction breaks the integrability of each commuting SYK and the family of models demonstrates the emergence of quantum chaos. We study the spectrum of this model analytically in the double-scaled limit. As the number of copies tends to infinity, the spectrum becomes compact and equivalent to the regular SYK model. For finite <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"><a:mi>d</a:mi></a:math> copies, the spectrum is close to the regular SYK model in UV but has an exponential tail <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"><c:msup><c:mi>e</c:mi><c:mrow><c:mi>E</c:mi><c:mo>/</c:mo><c:msub><c:mi>T</c:mi><c:mi>c</c:mi></c:msub></c:mrow></c:msup></c:math> in the IR. We identify the reciprocal of the exponent in the tail as a critical temperature <e:math xmlns:e="http://www.w3.org/1998/Math/MathML" display="inline"><e:msub><e:mi>T</e:mi><e:mi>c</e:mi></e:msub></e:math>, above which the model should be quantum chaotic. <g:math xmlns:g="http://www.w3.org/1998/Math/MathML" display="inline"><g:msub><g:mi>T</g:mi><g:mi>c</g:mi></g:msub></g:math> monotonically decreases as <i:math xmlns:i="http://www.w3.org/1998/Math/MathML" display="inline"><i:mi>d</i:mi></i:math> increases, which expands the chaotic regime over the nonchaotic regime. We propose the existence of a new phase around <k:math xmlns:k="http://www.w3.org/1998/Math/MathML" display="inline"><k:msub><k:mi>T</k:mi><k:mi>c</k:mi></k:msub></k:math>, and the dynamics should be very different in two phases. We further carry out numeric analysis at finite <m:math xmlns:m="http://www.w3.org/1998/Math/MathML" display="inline"><m:mi>d</m:mi></m:math>, which supports our proposal. Given any finite dimensional local Hamiltonian, by decomposing it into <o:math xmlns:o="http://www.w3.org/1998/Math/MathML" display="inline"><o:mi>d</o:mi></o:math> groups, in which all terms in one group commute with each other but terms from different groups may not, our analysis can give an estimate of the critical temperature for quantum chaos based on the decomposition. We also comment on the implication of the critical temperature to future quantum simulations of quantum chaos and quantum gravity.

Physical review. D/Physical review. D.Vol. 112(6)
Rutgers Sexual and Reproductive Health and Rights (NL), Kavli Institute for Theoretical Sciences (CN), Peng Huanwu Center for Fundamental Theory (CN)
Openalex Percentile: Top 6%
Nonlinear Waves and Solitons
3.97
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