Abstract
We identify a phase transition between two kinds of volume-law entangled phases in non-local but few-body unitary dynamics with local projective measurements. In one phase, a finite fraction of the system belongs to a fully-entangled state, one for which no subsystem is in a pure state, while in the second phase, the steady-state is a product state over extensively many, finite subsystems. We study this "separability" transition in a family of solvable models in which we analytically determine the transition point, the evolution of certain entanglement properties of interest, and relate this to a mean-field percolation transition. Since the entanglement entropy density does not distinguish these phases, we introduce the entangling power - which measures whether local measurements outside of two finite subsystems can boost their mutual information - as an order parameter, after considering its behavior in tensor network states, and numerically studying its behavior in a model of Clifford dynamics with measurements. We argue that in our models, the separability transition coincides with a transition in the computational "hardness" of classically determining the output probability distribution for the steady-state in a certain basis of product states. A prediction for this distribution, which is accurate in the separable phase, and should deviate from the true distribution in the fully-entangled phase, provides a possible benchmarking task for quantum computers.
Connections
Explore this paper’s authors, topics and related work.
Building this map preview
BZPEER is loading the nearby papers, people, topics and institutions for this page.
Reviews 0
Write a review
No reviews yet.
Discussion 0
Add a comment
No comments yet.