Clustering theorem in 1D long-range interacting systems at arbitrary temperatures
arXiv:2403.11431 · doi:10.1007/s00220-025-05242-4
Abstract
This paper delves into a fundamental aspect of quantum statistical mechanics -- the absence of thermal phase transitions in one-dimensional (1D) systems. Originating from Ising's analysis of the 1D spin chain, this concept has been pivotal in understanding 1D quantum phases, especially those with finite-range interactions as extended by Araki. In this work, we focus on quantum long-range interactions and successfully derive a clustering theorem applicable to a wide range of interaction decays at arbitrary temperatures. This theorem applies to any interaction forms that decay faster than and does not rely on translation invariance or infinite system size assumptions. Also, we rigorously established that the temperature dependence of the correlation length is given by , which is the same as the classical cases. Our findings indicate the absence of phase transitions in 1D systems with super-polynomially decaying interactions, thereby expanding upon previous theoretical research. To overcome significant technical challenges originating from the divergence of the imaginary-time Lieb-Robinson bound, we utilize the quantum belief propagation to refine the cluster expansion method. This approach allowed us to address divergence issues effectively and contributed to a deeper understanding of low-temperature behaviors in 1D quantum systems.
35 pages, 5 figures,
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Cited by in corpus (6)
- Rapid thermalization of dissipative many-body dynamics of commuting Hamiltonians
- Clustering of conditional mutual information and quantum Markov structure at arbitrary temperatures
- Provably Efficient Simulation of 1D Long-Range Interacting Systems at Any Temperature
- Stability of thermal equilibrium in long-range quantum systems
- High-temperature partition functions and classical simulatability of long-range quantum systems
- Efficient and simple Gibbs state preparation of the 2D toric code via duality to classical Ising chains