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This research establishes rigorous geometric lower bounds for one-dimensional chiral systems at finite temperatures, bridging the gap between zero-temperature topological invariants and high-temperature regimes using Uhlmann's framework. By verifying these findings with the SSH and Kitaev chain models, the study provides a theoretical foundation for detecting density matrix geometry within quantum circuits via the QITE method. These results advance our understanding of how geometric phases persist under thermal noise, which is critical for developing robust topological quantum error correction protocols.
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Quantum geometric bounds at finite temperature for one-dimensional chiral systems

arXiv2 min read

arXiv:2608.27944v1 Announce Type: cross Abstract: The geometry and topology of quantum states are intimately related at zero temperature through exact bounds that constrain geometric quantities from below by topological invariants. At finite-temperature, however, the analogous relations remain unclear. Here we establish rigorous geometric lower bounds for one-dimensional (1D) chiral-symmetric systems at finite temperature within the Uhlmann's framework for mixed states. We show that the Bures length is bounded by a continuous geometric phase angle. We further derive a temperature-dependent bound that interpolates between the zero-temperature limit and a trivial high-temperature regime. Our results are verified analytically and numerically using the Su-Schrieffer-Heeger (SSH) model and the spinless Kitaev chain model. Finally, we discuss potential ways to detect the geometry of the density matrix in quantum circuits, with the quantum imaginary time evolution (QITE) method.

Abstract:The geometry and topology of quantum states are intimately related at zero temperature through exact bounds that constrain geometric quantities from below by topological invariants. At finite-temperature, however, the analogous relations remain unclear. Here we establish rigorous geometric lower bounds for one-dimensional (1D) chiral-symmetric systems at finite temperature within the Uhlmann's framework for mixed states. We show that the Bures length is bounded by a continuous geometric phase angle. We further derive a temperature-dependent bound that interpolates between the zero-temperature limit and a trivial high-temperature regime. Our results are verified analytically and numerically using the Su-Schrieffer-Heeger (SSH) model and the spinless Kitaev chain model. Finally, we discuss potential ways to detect the geometry of the density matrix in quantum circuits, with the quantum imaginary time evolution (QITE) method.

Mesoscale and Nanoscale Physics (cond-mat.mes-hall); Quantum Physics (quant-ph)

arXiv:2608.27944 [cond-mat.mes-hall]

(or arXiv:2608.27944v1 [cond-mat.mes-hall] for this version)

https://doi.org/10.48550/arXiv.2608.27944 Focus to learn more arXiv-issued DOI via DataCite (pending registration)

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