{ "id": "2307.11609", "version": "v1", "published": "2023-07-21T14:25:22.000Z", "updated": "2023-07-21T14:25:22.000Z", "title": "Persistent Ballistic Entanglement Spreading with Optimal Control in Quantum Spin Chains", "authors": [ "Ying Lu", "Pei Shi", "Xiao-Han Wang", "Jie Hu", "Shi-Ju Ran" ], "comment": "5 pages, 4 figures", "categories": [ "quant-ph", "cond-mat.str-el", "cs.LG" ], "abstract": "Entanglement propagation provides a key routine to understand quantum many-body dynamics in and out of equilibrium. In this work, we uncover that the ``variational entanglement-enhancing'' field (VEEF) robustly induces a persistent ballistic spreading of entanglement in quantum spin chains. The VEEF is time dependent, and is optimally controlled to maximize the bipartite entanglement entropy (EE) of the final state. Such a linear growth persists till the EE reaches the genuine saturation $\\tilde{S} = - \\log_{2} 2^{-\\frac{N}{2}}=\\frac{N}{2}$ with $N$ the total number of spins. The EE satisfies $S(t) = v t$ for the time $t \\leq \\frac{N}{2v}$, with $v$ the velocity. These results are in sharp contrast with the behaviors without VEEF, where the EE generally approaches a sub-saturation known as the Page value $\\tilde{S}_{P} =\\tilde{S} - \\frac{1}{2\\ln{2}}$ in the long-time limit, and the entanglement growth deviates from being linear before the Page value is reached. The dependence between the velocity and interactions is explored, with $v \\simeq 2.76$, $4.98$, and $5.75$ for the spin chains with Ising, XY, and Heisenberg interactions, respectively. We further show that the nonlinear growth of EE emerges with the presence of long-range interactions.", "revisions": [ { "version": "v1", "updated": "2023-07-21T14:25:22.000Z" } ], "analyses": { "keywords": [ "quantum spin chains", "persistent ballistic entanglement spreading", "optimal control", "understand quantum many-body dynamics", "page value" ], "note": { "typesetting": "TeX", "pages": 5, "language": "en", "license": "arXiv", "status": "editable" } } }