2006
DOI: 10.1080/00018730600766432
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New trends in density matrix renormalization

Abstract: The Density Matrix Renormalization Group (DMRG) has become a powerful numerical method that can be applied to low-dimensional strongly correlated fermionic and bosonic systems. It allows for a very precise calculation of static, dynamic and thermodynamic properties. Its field of applicability has now extended beyond Condensed Matter, and is successfully used in Quantum Chemistry, Statistical Mechanics, Quantum Information Theory, Nuclear and High Energy Physics as well. In this article, we briefly review the m… Show more

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Cited by 353 publications
(251 citation statements)
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References 526 publications
(473 reference statements)
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“…In contrast to traditional vMPS approaches to disordered systems, where the initial geometry of the MPS ignores the disorder and only takes it into account at the stage of variational sweeps [45], our approach incorporates the disorder into the fabric of its tensor network. We believe this strategy to be inherently more suited to disordered systems-the results presented here show that the accuracy of tSDRG is already comparable to vMPS without including any additional variational updates.…”
Section: Discussionmentioning
confidence: 99%
“…In contrast to traditional vMPS approaches to disordered systems, where the initial geometry of the MPS ignores the disorder and only takes it into account at the stage of variational sweeps [45], our approach incorporates the disorder into the fabric of its tensor network. We believe this strategy to be inherently more suited to disordered systems-the results presented here show that the accuracy of tSDRG is already comparable to vMPS without including any additional variational updates.…”
Section: Discussionmentioning
confidence: 99%
“…There, the recent algorithms introduced by Vidal 1 based on the explicit use of Schmidt decompositions have been shown to deliver identical results to the very successful density matrix renormalization group ͑DMRG͒. [2][3][4] Actually, these two apparently wide-apart algorithms agree because they come down to represent the coefficients of a quantum state as a product of matrices, which is a matrix product state ͑MPS͒, 5 where s i labels a basis for the local degree of freedom ͑"spin"͒ of particle i, A i ͑s i ͒'s are matrices of some fixed finite size, , and N is the number of sites in the chain which will be taken to be infinite. 8 Under the assumption that the abovementioned algorithms do find a faithful description of the sought state, consistent with the MPS structure, we can forget about their details and describe their results as a consequence of the properties of MPS states.…”
Section: Introductionmentioning
confidence: 95%
“…We fit the local spin polarization s z l and the longitudinal spin fluctuation correlation s z l s z l ′ − s z l s z l ′ to Eqs. (36) and (44) with p = 3, respectively, taking η and a as fitting parameters. We find that these correlators are fitted quite well by the formulas.…”
Section: Triatic and Quartic Phasesmentioning
confidence: 99%
“…29,30,31,32 In this paper we concentrate on the ferromagnetic case (J 1 < 0) of the J 1 -J 2 spin chain (1) in magnetic field which partially polarizes spins to the +z direction. We show that the ground-state phase diagram in the case is a zoo of exotic quantum phases, using the numerical density-matrix renormalization group (DMRG) method, 33,34,35,36 exact-diagonalization method, and effective field theories. We find a phase with long-range vector chiral order and phases with various kinds of multipolar spin correlations, most of which have not been known to appear in this model.…”
Section: Introductionmentioning
confidence: 99%