2017
DOI: 10.1103/physrevb.95.195148
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Symmetric minimally entangled typical thermal states for canonical and grand-canonical ensembles

Abstract: Based on the density matrix renormalization group (DMRG), strongly correlated quantum manybody systems at finite temperatures can be simulated by sampling over a certain class of pure matrix product states (MPS) called minimally entangled typical thermal states (METTS). When a system features symmetries, these can be utilized to substantially reduce MPS computation costs. It is conceptually straightforward to simulate canonical ensembles using symmetric METTS. In practice, it is important to alternate between … Show more

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Cited by 25 publications
(16 citation statements)
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References 34 publications
(60 reference statements)
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“…The explicit implementation of non-Abelian symmetries has been regarded as a standard technique in ground state DMRG simulations (T = 0) [43], which has many important applications including exploring quantum spin liquids in frustrated quantum magnets [44,45], and is also shown to be useful in METTS-type thermal simulations [46,47]. However, the implementations of non-Abelian symmetries in MPO for finite-temperature simulations are still absent.…”
Section: A Symmetric Matrix Product Operatormentioning
confidence: 99%
“…The explicit implementation of non-Abelian symmetries has been regarded as a standard technique in ground state DMRG simulations (T = 0) [43], which has many important applications including exploring quantum spin liquids in frustrated quantum magnets [44,45], and is also shown to be useful in METTS-type thermal simulations [46,47]. However, the implementations of non-Abelian symmetries in MPO for finite-temperature simulations are still absent.…”
Section: A Symmetric Matrix Product Operatormentioning
confidence: 99%
“…Secondly, because METTS updates remain in a fixed quantum-number sector corresponding to the symmetries of the Hamiltonian, one cannot straightforwardly use quantum numbers to simulate the grand canonical ensemble efficiently [12,13]. On the contrary, using purification, the maximally entangled state |S allows particle numbers to fluctuate on the physical sites while keeping the total number of particles conserved in the total space (physical and auxiliary).…”
Section: Hybrid Algorithmmentioning
confidence: 99%
“…Apart from the imaginary time evolution itself, the main challenge in obtaining the Matsubara Green function is computing finite temperature versus ground state properties. Within tensor network methods, finite temperature systems can be accessed in two ways: (i) the minimally entangled typical thermal states (METTS) algorithm [11][12][13][14][15] uses a sampling technique over tensor network states to produce the thermal average; (ii) the purification technique [16][17][18][19] rewrites the thermal trace as a average in a pure state in a larger space, obtained by imaginary time evolution.…”
Section: Introductionmentioning
confidence: 99%
“…For efficient sampling in the vast Hilbert space, the sampling approach is often combined with the importance sampling implemented by the Markov chain. However, there is a drawback in the use of the Markov chain that it can bring the autocorrelation problem [17], and thus some treatments to circumvent the problem are required in such approaches [15,16,[18][19][20][21][22].…”
Section: Introductionmentioning
confidence: 99%