Phase transition extracted by principal component analysis in the disordered Moore–Read state

Abstract We study the influence of disorder on the Moore–Read state by principal component analysis (PCA), which is one of the ground state candidates for the 5/2 fractional Hall state. By using PCA, the topological features of the ground state wave functions with different disorder strengths can be distilled. As the disorder strength increases, the Moore–Read state will be destroyed. We explore the phase transition by analyzing the overlaps between the random sample wave functions and the topologically distilled state. The cross-point between the amplitudes of the principal component and its counterpart is the phase transition point. Additionally, the origin of the second component comes from the excited states, which is different from the Laughlin state.

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Publication Details

Journal
Chinese Physics B
Published
2025-02-05
DOI
https://doi.org/10.1088/1674-1056/adb25f
Primary Topic
Theoretical and Computational Physics
Type
article
Field-Weighted Citation Impact
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article

Phase transition extracted by principal component analysis in the disordered Moore–Read state

Na Jiang, Zheng Ma, L. M. Wang, S. H. 少华 Fu 付
Chinese Physics B
Theoretical and Computational Physics
article

Phase transition extracted by principal component analysis in the disordered Moore–Read state

Na Jiang, Zheng Ma, L. M. Wang, S. H. 少华 Fu 付
article en

Abstract

Abstract We study the influence of disorder on the Moore–Read state by principal component analysis (PCA), which is one of the ground state candidates for the 5/2 fractional Hall state. By using PCA, the topological features of the ground state wave functions with different disorder strengths can be distilled. As the disorder strength increases, the Moore–Read state will be destroyed. We explore the phase transition by analyzing the overlaps between the random sample wave functions and the topologically distilled state. The cross-point between the amplitudes of the principal component and its counterpart is the phase transition point. Additionally, the origin of the second component comes from the excited states, which is different from the Laughlin state.

Chinese Physics BVol. 34(4)
Chongqing University (CN), Chongqing Jiaotong University (CN)
Openalex Percentile: Top 99%
Theoretical and Computational Physics
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