2021
DOI: 10.48550/arxiv.2109.01619
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Exploring Finite Temperature Properties of Materials with Quantum Computers

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Cited by 4 publications
(4 citation statements)
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“…III B was used to calculate dynamical spin-spin correlation functions in a driven Floquet spin chain in order to verify the occurrence of discrete time-crystalline eigenstate order. Moreover, in [179], quantum typicality was used to evaluate thermodynamic expectation values at finite temperature (cf. Box 2), which involved the approximation of the imaginary time-evolution of random states on a NISQ device [180].…”
Section: Discussionmentioning
confidence: 99%
“…III B was used to calculate dynamical spin-spin correlation functions in a driven Floquet spin chain in order to verify the occurrence of discrete time-crystalline eigenstate order. Moreover, in [179], quantum typicality was used to evaluate thermodynamic expectation values at finite temperature (cf. Box 2), which involved the approximation of the imaginary time-evolution of random states on a NISQ device [180].…”
Section: Discussionmentioning
confidence: 99%
“…The Heisenberg model is of fundamental importance in the study of quantum materials [39][40][41][42] and is therefore a standard benchmark for thermal state preparation methods [29,30,43].…”
Section: B Transverse Field Ising Chainmentioning
confidence: 99%
“…One promising route to quantum computing thermal systems is the thermal pure-quantum-(TPQ-) state formulation of statistical mechanics [21]. While originally developed without quantum technology in mind, this ansatz offers a promising route to simulating quantum systems at finite temperature and chemical potential, enabling estimations of thermal expectation values of a large class of observables from only a single properly prepared pure state in the thermodynamic limit [22,23]. Canonical TPQ states are obtained from a Haar-random state evolved in imaginary time [21],…”
Section: Introductionmentioning
confidence: 99%