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arXiv:1602.04380 · Physical review. B./Physical review. B

Entanglement entropy of disordered quantum chains following a global quench

Yang Zhao, F. Andraschko, Jesko Sirker

Published May 25, 2016• 43 citations
arXivHTMLPDF

Abstract

We numerically investigate the growth of the entanglement entropy ${S}_{\mathrm{ent}}(t)$ in time $t$, after a global quench from a product state, in quantum chains with various kinds of disorder. The main focus is, in particular, on fermionic chains with bond disorder. In the noninteracting case at criticality we numerically test recent predictions by the real-space renormalization group for the entanglement growth in time, the maximal entanglement as a function of block size, and the decay of a density-wave order parameter. We show that multiprecision calculations are required to reach the scaling regime and perform such calculations for specific cases. For interacting models with binary bond disorder we present data based on infinite-size density matrix renormalization group calculations and exact diagonalizations. We obtain numerical evidence of a many-body localized phase in bond-disordered systems where ${S}_{\mathrm{ent}}(t)\ensuremath{\sim}lnt$ seems to hold. Our results for bond disorder are contrasted with the well-studied case of potential disorder.

DOI
10.1103/physrevb.93.205146

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We numerically investigate the growth of the entanglement entropy Sent(t){S}_{\mathrm{ent}}(t)Sent​(t) in time ttt, after a global quench from a product state, in quantum chains with various kinds of disorder. The main focus is, in particular, on fermionic chains with bond disorder. In the noninteracting case at criticality we numerically test recent predictions by the real-space renormalization group for the entanglement growth in time, the maximal entanglement as a function of block size, and the decay of a density-wave order parameter. We show that multiprecision calculations are required to reach the scaling regime and perform such calculations for specific cases. For interacting models with binary bond disorder we present data based on infinite-size density matrix renormalization group calculations and exact diagonalizations. We obtain numerical evidence of a many-body localized phase in bond-disordered systems where Sent(t)\ensuremath∼lnt{S}_{\mathrm{ent}}(t)\ensuremath{\sim}lntSent​(t)\ensuremath∼lnt seems to hold. Our results for bond disorder are contrasted with the well-studied case of potential disorder.
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We investigate the growth of the entanglement entropy Sent{S}_{\mathrm{ent}}Sent​ following global quenches in two-dimensional free fermion models with potential and bond disorder. For the potential disorder case, we show that an intermediate weak localization regime exists in which Sent(t){S}_{\mathrm{ent}}(t)Sent​(t) grows logarithmically in time ttt before Anderson localization sets in. For the case of binary bond disorder near the percolation transition, we find additive logarithmic corrections to area and volume laws as well as a scaling at long times, which is consistent with an infinite randomness fixed point.
We study the growth of entanglement entropy in density-matrix renormalization-group calculations of the real-time quench dynamics of the Anderson impurity model. We find that with an appropriate choice of basis, the entropy growth is logarithmic in both the interacting and noninteracting single-impurity models. The logarithmic entropy growth is understood from a noninteracting chain model as a critical behavior separating regimes of linear growth and saturation of entropy, which correspond respectively to overlapping and gapped energy spectra of the set of bath states. We find that a logarithmic entropy growth is the generic behavior of quenched impurity models when the bath orbitals in the matrix product state are ordered in energy. A noninteracting calculation of the double-impurity Anderson model supports the conclusion in the multi-impurity case. The logarithmic growth of entanglement entropy enables studies of quench dynamics to very long times.
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By means of free fermionic techniques we study the time evolution of the entanglement entropy S(t)\mathcal{S}(t)S(t) of a block of spins in the random transverse-field Ising chain after a sudden change of the parameters of the Hamiltonian. We consider global quenches, when the parameters are modified uniformly in space, as well as local quenches, when two disconnected blocks are suddenly joined together. For a noncritical final state, the dynamical entanglement entropy is found to approach a finite limiting value for both types of quenches. If the quench is performed to the critical state, the entropy grows for an infinite block as $\mathcal{S}(t)\ensuremath{\sim}\mathrm{ln}\mathrm{ln}t$. This type of ultraslow increase is explained through the strong disorder renormalization group method.