Krylov complexity in 2d CFTs with SL(2, ℝ) deformed Hamiltonians

A bstract In this study, we analyze Krylov Complexity in two-dimensional conformal field theories subjected to deformed SL(2 , ℝ) Hamiltonians. In the Vacuum state, we find that the K-Complexity exhibits a universal phase structure. The phase structure involves the K-Complexity exhibiting an oscillatory behaviour in the non-heating phase, which contrasts with the exponential growth observed in the heating phase, while it displays polynomial growth at the phase boundary. Furthermore, we extend our analysis to compute the K-Complexity of a light operator in excited states, considering both large-c CFT and free field theory. In the free field theory, we find a state-independent phase structure of K-Complexity. However, in the large-c CFT, the behaviour varies, with the K-Complexity once again displaying exponential growth in the heating phase and polynomial growth at the phase boundary. Notably, the precise exponent governing this growth depends on the heaviness of the state under examination. In the non-heating phase, we observe a transition in K-Complexity behaviour from oscillatory to exponential growth, akin to findings in [1], as it represents a special case within the non-heating phase.

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Publication Details

Journal
Journal of High Energy Physics
Published
2025-02-06
DOI
https://doi.org/10.1007/jhep02(2025)035
Citations
12
Primary Topic
Quantum many-body systems
Type
article
Field-Weighted Citation Impact
14.96

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article

Krylov complexity in 2d CFTs with SL(2, ℝ) deformed Hamiltonians

Vinay Malvimat, Baishali Roy, Somnath Porey
12 citations
Journal of High Energy Physics
Quantum many-body systems
14.96
article

Krylov complexity in 2d CFTs with SL(2, ℝ) deformed Hamiltonians

Vinay Malvimat, Baishali Roy, Somnath Porey
article en
12 citations

Abstract

A bstract In this study, we analyze Krylov Complexity in two-dimensional conformal field theories subjected to deformed SL(2 , ℝ) Hamiltonians. In the Vacuum state, we find that the K-Complexity exhibits a universal phase structure. The phase structure involves the K-Complexity exhibiting an oscillatory behaviour in the non-heating phase, which contrasts with the exponential growth observed in the heating phase, while it displays polynomial growth at the phase boundary. Furthermore, we extend our analysis to compute the K-Complexity of a light operator in excited states, considering both large-c CFT and free field theory. In the free field theory, we find a state-independent phase structure of K-Complexity. However, in the large-c CFT, the behaviour varies, with the K-Complexity once again displaying exponential growth in the heating phase and polynomial growth at the phase boundary. Notably, the precise exponent governing this growth depends on the heaviness of the state under examination. In the non-heating phase, we observe a transition in K-Complexity behaviour from oscillatory to exponential growth, akin to findings in [1], as it represents a special case within the non-heating phase.

Journal of High Energy PhysicsVol. 2025(2)
Asia Pacific Center for Theoretical Physics (KR), Ramakrishna Mission Vivekananda Educational and Research Institute (IN)
National Research Foundation, National Research Foundation of Korea, Yukawa Institute for Theoretical Physics, Kyoto University, Ministry of Science and ICT, South Korea
Openalex Percentile: Top 1%
Quantum many-body systems
14.96
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