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arXiv:1501.02852 · Physical Review B

Generalized mutual information of quantum critical chains

Francisco Castilho Alcaraz, M. A. Rajabpour

Published Apr 15, 2015• 27 citations
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Abstract

We study the generalized mutual information ${\stackrel{\ifmmode \tilde{}\else \~{}\fi{}}{I}}_{n}$ of the ground state of different critical quantum chains. The generalized mutual information definition that we use is based on the well established concept of the R\'enyi divergence. We calculate this quantity numerically for several distinct quantum chains having either discrete $Z(Q)$ symmetries ($Q$-state Potts model with $Q=2,3,4$ and $Z(Q)$ parafermionic models with $Q=5,6,7,8$ and also Ashkin-Teller model with different anisotropies) or the $U(1)$ continuous symmetries (Klein-Gordon field theory, $XXZ$ and spin-1 Fateev-Zamolodchikov quantum chains with different anisotropies). For the spin chains these calculations were done by expressing the ground-state wave functions in two special bases. Our results indicate some general behavior for particular ranges of values of the parameter $n$ that defines ${\stackrel{\ifmmode \tilde{}\else \~{}\fi{}}{I}}_{n}$. For a system, with total size $L$ and subsystem sizes $\ensuremath{\ell}$ and $L\ensuremath{-}\ensuremath{\ell}$, the ${\stackrel{\ifmmode \tilde{}\else \~{}\fi{}}{I}}_{n}$ has a logarithmic leading behavior given by $\frac{{\stackrel{\ifmmode \tilde{}\else \~{}\fi{}}{c}}_{n}}{4}log[\frac{L}{\ensuremath{\pi}}sin(\frac{\ensuremath{\pi}\ensuremath{\ell}}{L})]$ where the coefficient ${\stackrel{\ifmmode \tilde{}\else \~{}\fi{}}{c}}_{n}$ is linearly dependent on the central charge $c$ of the underlying conformal field theory describing the system's critical properties.

DOI
10.1103/physrevb.91.155122

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We study the generalized mutual information I\ifmmode~\else˜\fin{\stackrel{\ifmmode \tilde{}\else \~{}\fi{}}{I}}_{n}I\ifmmode~\else˜\fi​n​ of the ground state of different critical quantum chains. The generalized mutual information definition that we use is based on the well established concept of the R'enyi divergence. We calculate this quantity numerically for several distinct quantum chains having either discrete Z(Q)Z(Q)Z(Q) symmetries (QQQ-state Potts model with Q=2,3,4Q=2,3,4Q=2,3,4 and Z(Q)Z(Q)Z(Q) parafermionic models with Q=5,6,7,8Q=5,6,7,8Q=5,6,7,8 and also Ashkin-Teller model with different anisotropies) or the U(1)U(1)U(1) continuous symmetries (Klein-Gordon field theory, XXZXXZXXZ and spin-1 Fateev-Zamolodchikov quantum chains with different anisotropies). For the spin chains these calculations were done by expressing the ground-state wave functions in two special bases. Our results indicate some general behavior for particular ranges of values of the parameter nnn that defines I\ifmmode~\else˜\fin{\stackrel{\ifmmode \tilde{}\else \~{}\fi{}}{I}}_{n}I\ifmmode~\else˜\fi​n​. For a system, with total size LLL and subsystem sizes \ensuremathℓ\ensuremath{\ell}\ensuremathℓ and L\ensuremath−\ensuremathℓL\ensuremath{-}\ensuremath{\ell}L\ensuremath−\ensuremathℓ, the I\ifmmode~\else˜\fin{\stackrel{\ifmmode \tilde{}\else \~{}\fi{}}{I}}_{n}I\ifmmode~\else˜\fi​n​ has a logarithmic leading behavior given by c\ifmmode~\else˜\fin4log[L\ensuremathπsin(\ensuremathπ\ensuremathℓL)]\frac{{\stackrel{\ifmmode \tilde{}\else \~{}\fi{}}{c}}_{n}}{4}log[\frac{L}{\ensuremath{\pi}}sin(\frac{\ensuremath{\pi}\ensuremath{\ell}}{L})]4c\ifmmode~\else˜\fin​​log[\ensuremathπL​sin(L\ensuremathπ\ensuremathℓ​)] where the coefficient c\ifmmode~\else˜\fin{\stackrel{\ifmmode \tilde{}\else \~{}\fi{}}{c}}_{n}c\ifmmode~\else˜\fin​ is linearly dependent on the central charge ccc of the underlying conformal field theory describing the system's critical properties.
We study the Shannon and R\'enyi mutual information (MI) in the ground state (GS) of different critical quantum spin chains. Despite the apparent basis dependence of these quantities we show the existence of some particular basis (we will call them conformal basis) whose finite-size scaling function is related to the central charge ccc of the underlying conformal field theory of the model. In particular, we verified that for large index nnn, the MI of a subsystem of size $\ensuremath{\ell}$ in a periodic chain with LLL sites behaves as $\frac{c}{4}\frac{n}{n\ensuremath{-}1}ln[\frac{L}{\ensuremath{\pi}}sin(\frac{\ensuremath{\pi}\ensuremath{\ell}}{L})]$, when the ground-state wave function is expressed in these special conformal basis. This is in agreement with recent predictions. For generic local basis, we will show that, although in some cases ${b}_{n}ln[\frac{L}{\ensuremath{\pi}}sin(\frac{\ensuremath{\pi}\ensuremath{\ell}}{L})]$ is a good fit to our numerical data, in general, there is no direct relation between bn{b}_{n}bn​ and the central charge of the system. We will support our findings with detailed numerical calculations for the transverse field Ising model, Q=3,4Q=3,4Q=3,4 quantum Potts chain, quantum Ashkin-Teller chain, and the XXZ quantum chain. We will also present some additional results of the Shannon mutual information (n=1n=1n=1), for the parafermionic ZQ{Z}_{Q}ZQ​ quantum chains with Q=5,6,7Q=5,6,7Q=5,6,7, and 8.
An existing conjecture states that the Shannon mutual information contained in the ground-state wave function of conformally invariant quantum chains, on periodic lattices, has a leading finite-size scaling behavior that, similarly as the von Neumann entanglement entropy, depends on the value of the central charge of the underlying conformal field theory describing the physical properties. This conjecture applies whenever the ground-state wave function is expressed in some special basis (conformal basis). Its formulation comes mainly from numerical evidences on exactly integrable quantum chains. In this paper, the above conjecture was tested for several general nonintegrable quantum chains. We introduce new families of self-dual Z(Q)Z(Q)Z(Q) symmetric quantum chains (Q=2,3,...)(Q=2,3,...)(Q=2,3,...). These quantum chains contain nearest-neighbor as well next-nearest-neighbor interactions (coupling constant p)p)p). In the cases Q=2Q=2Q=2 and Q=3Q=3Q=3, they are extensions of the standard quantum Ising and three-state Potts chains, respectively. For Q=4Q=4Q=4 and $Q\ensuremath{\ge}5$, they are extensions of the Ashkin-Teller and Z(Q)Z(Q)Z(Q) parafermionic quantum chains. Our studies indicate that these models are interesting on their own. They are critical, conformally invariant, and share the same universality class in a continuous critical line. Moreover, our numerical analysis for Q=2−−8Q=2--8Q=2−−8 indicate that the Shannon mutual information exhibits the conjectured behavior irrespective if the conformally invariant quantum chain is exactly integrable or not. For completeness we also calculated, for these new families of quantum chains, the two existing generalizations of the Shannon mutual information, which are based on the R\'enyi entropy and on the R\'enyi divergence.
We consider the Shannon mutual information of subsystems of critical quantum chains in their ground states. Our results indicate a universal leading behavior for large subsystem sizes. Moreover, as happens with the entanglement entropy, its finite-size behavior yields the conformal anomaly c of the underlying conformal field theory governing the long-distance physics of the quantum chain. We study analytically a chain of coupled harmonic oscillators and numerically the Q-state Potts models (Q=2, 3, and 4), the XXZ quantum chain, and the spin-1 Fateev-Zamolodchikov model. The Shannon mutual information is a quantity easily computed, and our results indicate that for relatively small lattice sizes, its finite-size behavior already detects the universality class of quantum critical behavior.
Using the density matrix renormalization group, we calculated the finite-size corrections of the entanglement $\ensuremath{\alpha}$-R\'enyi entropy of a single interval for several critical quantum chains. We considered models with U(1)U(1)U(1) symmetry such as the spin-1/2 XXZXXZXXZ and spin-1 Fateev-Zamolodchikov models, as well as models with discrete symmetries such as the Ising, the Blume-Capel, and the three-state Potts models. These corrections contain physically relevant information. Their amplitudes, which depend on the value of $\ensuremath{\alpha}$, are related to the dimensions of operators in the conformal field theory governing the long-distance correlations of the critical quantum chains. The obtained results together with earlier exact and numerical ones allow us to formulate some general conjectures about the operator responsible for the leading finite-size correction of the $\ensuremath{\alpha}$-R\'enyi entropies. We conjecture that the exponent of the leading finite-size correction of the $\ensuremath{\alpha}$-R\'enyi entropies is ${p}_{\ensuremath{\alpha}}=2{X}_{\ensuremath{\epsilon}}/\ensuremath{\alpha}$ for $\ensuremath{\alpha}>1$ and ${p}_{1}=\ensuremath{\nu}$, where ${X}_{\ensuremath{\epsilon}}$ denotes the dimensions of the energy operator of the model and $\ensuremath{\nu}=2$ for all the models.
We study the mutual information between two lattice blocks in terms of von Neumann entropies for one-dimensional infinite lattice systems. Quantum q-state Potts model and transverse-field spin-1/2 XY model are considered numerically by using the infinite matrix product state approach. As a system parameter varies, block-block mutual information exhibit singular behaviors that enable us to identify the critical points for the quantum phase transitions. As happens with von Neumann entanglement entropy of single block, at critical points, block-block mutual information for two adjacent blocks show a logarithmic leading behavior with increasing the size of the blocks, which yields the central charge c of the underlying conformal field theory, as it should be. It seems that two disjoint blocks show a similar logarithmic growth of the mutual information as a characteristic property of critical systems but the proportional coefficients of the logarithmic term are very different from the central charges. As the separation between the two lattice blocks increases, the mutual information reveals a consistent power-law decaying behavior for various truncation dimensions and lattice-block sizes. The critical exponent of block-block mutual information in the thermodynamic limit is estimated by extrapolating the exponents of power-law decaying regions for finite truncation dimensions. For a given lattice-block size ℓ, the critical exponents for the same universality classes seem to have very close values each other. Whereas the critical exponents have different values to a degree of distinction for the different universality classes. As the lattice-block size becomes bigger, the critical exponent becomes smaller. We discuss a relation between the exponents of block-block mutual information and correlation with the Shatten one-norm of block-block correlation.
We study mutual information for Renyi entropy of arbitrary index n, in interacting quantum systems at finite-temperature critical points, using high-temperature expansion, quantum Monte Carlo simulations and scaling theory. We find that, for n>1, the critical behavior is manifest at two temperatures T(c) and nT(c). For the XXZ model with Ising anisotropy, the coefficient of the area law has a t lnt singularity, whereas the subleading correction from corners has a logarithmic divergence, with a coefficient related to the exact results of Cardy and Peschel. For T<nT(c) there is a constant term associated with broken symmetries that jumps at both T(c) and nT(c), which can be understood in terms of a scaling function analogous to the boundary entropy of Affleck and Ludwig.