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arXiv:1708.07121 · Physical review. B./Physical review. B

Fisher information approach to nonequilibrium phase transitions in a quantum XXZ spin chain with boundary noise

Ugo Marzolino, Tomaž Prosen

Published Sep 1, 2017• 63 citations
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Abstract

We investigated quantum critical behaviors in the nonequilibrium steady state of a XXZ spin chain with boundary Markovian noise using Fisher information. The latter represents the distance between two infinitesimally close states, and its superextensive size scaling witnesses a critical behavior due to a phase transition since all the interaction terms are extensive. Perturbatively, in the noise strength, we found superextensive Fisher information at anisotropy $|\mathrm{\ensuremath{\Delta}}|\ensuremath{\leqslant}1$ and irrational $\frac{arccos\mathrm{\ensuremath{\Delta}}}{\ensuremath{\pi}}$ irrespective of the order of two noncommuting limits, i.e., the thermodynamic limit and the limit of sending $\frac{arccos\mathrm{\ensuremath{\Delta}}}{\ensuremath{\pi}}$ to an irrational number via a sequence of rational approximants. From this result we argue the existence of a nonequilibrium quantum phase transition with a critical phase $|\mathrm{\ensuremath{\Delta}}|\ensuremath{\leqslant}1$. From the nonsuperextensivity of the Fisher information of reduced states, we infer that this nonequilibrium quantum phase transition does not have local order parameters but has nonlocal ones, at least at $|\mathrm{\ensuremath{\Delta}}|=1$. In the nonperturbative regime for the noise strength, we numerically computed the reduced Fisher information which lower bounds the full-state Fisher information and is superextensive only at $|\mathrm{\ensuremath{\Delta}}|=1$. From the latter result, we derived local order parameters at $|\mathrm{\ensuremath{\Delta}}|=1$ in the nonperturbative case. The existence of critical behavior witnessed by the Fisher information in the phase $|\mathrm{\ensuremath{\Delta}}|<1$ is still an open problem. The Fisher information also represents the best sensitivity for any estimation of the control parameter, in our case the anisotropy $\mathrm{\ensuremath{\Delta}}$, and its superextensivity implies enhanced estimation precision which is also highly robust in the presence of a critical phase.

DOI
10.1103/physrevb.96.104402

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We investigated quantum critical behaviors in the nonequilibrium steady state of a XXZ spin chain with boundary Markovian noise using Fisher information. The latter represents the distance between two infinitesimally close states, and its superextensive size scaling witnesses a critical behavior due to a phase transition since all the interaction terms are extensive. Perturbatively, in the noise strength, we found superextensive Fisher information at anisotropy ∣\ensuremathΔ∣\ensuremath⩽1|\mathrm{\ensuremath{\Delta}}|\ensuremath{\leqslant}1∣\ensuremathΔ∣\ensuremath⩽1 and irrational arccos\ensuremathΔ\ensuremathπ\frac{arccos\mathrm{\ensuremath{\Delta}}}{\ensuremath{\pi}}\ensuremathπarccos\ensuremathΔ​ irrespective of the order of two noncommuting limits, i.e., the thermodynamic limit and the limit of sending arccos\ensuremathΔ\ensuremathπ\frac{arccos\mathrm{\ensuremath{\Delta}}}{\ensuremath{\pi}}\ensuremathπarccos\ensuremathΔ​ to an irrational number via a sequence of rational approximants. From this result we argue the existence of a nonequilibrium quantum phase transition with a critical phase ∣\ensuremathΔ∣\ensuremath⩽1|\mathrm{\ensuremath{\Delta}}|\ensuremath{\leqslant}1∣\ensuremathΔ∣\ensuremath⩽1. From the nonsuperextensivity of the Fisher information of reduced states, we infer that this nonequilibrium quantum phase transition does not have local order parameters but has nonlocal ones, at least at ∣\ensuremathΔ∣=1|\mathrm{\ensuremath{\Delta}}|=1∣\ensuremathΔ∣=1. In the nonperturbative regime for the noise strength, we numerically computed the reduced Fisher information which lower bounds the full-state Fisher information and is superextensive only at ∣\ensuremathΔ∣=1|\mathrm{\ensuremath{\Delta}}|=1∣\ensuremathΔ∣=1. From the latter result, we derived local order parameters at ∣\ensuremathΔ∣=1|\mathrm{\ensuremath{\Delta}}|=1∣\ensuremathΔ∣=1 in the nonperturbative case. The existence of critical behavior witnessed by the Fisher information in the phase ∣\ensuremathΔ∣<1|\mathrm{\ensuremath{\Delta}}|<1∣\ensuremathΔ∣<1 is still an open problem. The Fisher information also represents the best sensitivity for any estimation of the control parameter, in our case the anisotropy \ensuremathΔ\mathrm{\ensuremath{\Delta}}\ensuremathΔ, and its superextensivity implies enhanced estimation precision which is also highly robust in the presence of a critical phase.
The quantum Fisher information, the quantum analog of the classical Fisher information, is a central quantity in quantum metrology and quantum sensing due to its connection to parameter estimation and fidelity susceptibility. Using numerically exact methods applied to a paradigmatic open quantum system, the spin-boson model, we calculate both static and dynamical quantum Fisher information matrix elements with respect to spin-bath couplings and magnetic field strengths. As the spin-bath interaction increases, we first show that the coupling-coupling matrix elements relative to the ground state of the Hamiltonian are linked to the entanglement growth and signal the Berezinskii-Kosterlitz-Thouless quantum phase transition through their nonmonotonic behavior. We also point out that the static quantum Fisher information exhibits a nonperturbative behavior in the zero-coupling limit, which we justify with an analytic argument. Furthermore, we demonstrate that the time-dependent matrix elements can reveal non-Markovian effects as well as the transition from the coherent to incoherent regime at the Toulouse point, remaining robust under pure dephasing noise. Nonmonotonic signatures of the quantum Fisher information matrix reflect changes in quantum resources such as entanglement and coherence, quantify non-Markovian behavior, and enable criticality-enhanced quantum sensing, thereby shedding light on key features of open quantum systems.
We consider parameter estimations with probes being the boundary-driven or dissipated nonequilibrium steady states of XXZXXZXXZ spin-1/21/21/2 chains. The parameters to be estimated are the dissipation coupling and the anisotropy of the spin-spin interaction. In the weak-coupling regime we compute the scaling of the Fisher information, i.e., the inverse best sensitivity among all estimators, with the number of spins. We find superlinear scalings and transitions between the distinct isotropic and anisotropic phases. We also look at the best relative error, which decreases with the number of particles faster than the shot-noise only for the estimation of anisotropy.
Non-equilibrium phase transitions of open quantum systems generically exhibit diverging classical but not quantum correlations. Still entanglement -- characterizing the latter correlations -- can be sensitive to the phase transition. Furthermore, mutual information, bounding the total correlations, should exhibit critical scaling at the transition. In this work, we study these quantities in the steady state of open quantum Ising chains with power-law interactions (with the exponent 0≤α≤30\le α\le 30≤α≤3) where spins are subject to spontaneous emission. The bulk of this paper is dedicated to a detailed analytical as well as numerical analysis of the infinite-range model (α=0α=0α=0), a model that is closely related to the paradigmatic open Dicke model. Our main findings are that the entanglement, while being finite, peaks, exhibits a kink and takes a universal value at the transition, while the mutual information exhibits critical scaling not only at the transition but well into the ordered phase, underscoring a hidden criticality that is not captured by (two-point) correlations. We consider three distinct entanglement measures: logarithmic negativity; quantum Fisher information; and, spin squeezing. Specifically, we show that the collective spin operator that maximizes the quantum Fisher information can be identified with the \textit{gapless} mode of the phase transition, while the squeezed direction is that of the \textit{gapped} mode. Finally, we investigate power-law interacting models using matrix product states where we find comparable bounds on squeezing even when no phase transition is expected (for larger ααα), thus the connection to the phase transition does not appear to hold for shorter-range interactions.
In this paper, we study the ground-state quantum Fisher information (QFI) in one-dimensional spin-1 models, as witness to multipartite entanglement. The models addressed are the bilinear-biquadratic model, the most general isotropic SU(2)\text{SU}(2)SU(2)-invariant spin-1 chain, and the XXZXXZXXZ spin-1 chain, both with nearest-neighbor interactions and open boundary conditions. We show that the scaling of the QFI of strictly nonlocal observables can be used for characterizing the phase diagrams and, in particular, for studying topological phases, where it scales maximally. Analyzing its behavior at the critical phases, we are also able to recover the scaling dimensions of the order parameters, both for local and string observables. The numerical results have been obtained by exploiting the density-matrix renormalization-group algorithm and tensor network techniques.
In this paper, we investigate Quantum Phase Transitions (QPTs) in the long-range XXZ spin chain using two information-theoretic probes: The half-chain entanglement entropy and a witness of genuine multipartite nonlocality. Both quantities effectively identify the phase boundary, but exhibit distinct scaling behaviors: the entanglement entropy grows linearly with system size N, while the multipartite nonlocality increases exponentially, with [Formula: see text]. By independently tuning the power-law decay exponents of the transverse ([Formula: see text]) and longitudinal ([Formula: see text]) couplings, we uncover contrasting trends in the critical point [Formula: see text]: Increasing [Formula: see text] shifts it to larger values, while increasing [Formula: see text] shifts it to smaller ones. These monotonic and saturating dependencies are captured by an empirical exponential model, offering a compact and physically transparent description of the critical behavior. Our results highlight the crucial role of interaction range in driving criticality, with implications for engineered quantum systems and long-range entanglement control.