Guo Andrew Y, Tran Minh C, Childs Andrew M, Gorshkov Alexey V, Gong Zhe-Xuan
Joint Center for Quantum Information and Computer Science, NIST/University of Maryland, College Park, Maryland 20742, USA.
Joint Quantum Institute, NIST/University of Maryland, College Park, Maryland 20742, USA.
Phys Rev A (Coll Park). 2020;102. doi: 10.1103/PhysRevA.102.010401.
Strongly long-range interacting quantum systems-those with interactions decaying as a power law 1/ in the distance on a -dimensional lattice for ⩽ -have received significant interest in recent years. They are present in leading experimental platforms for quantum computation and simulation, as well as in theoretical models of quantum-information scrambling and fast entanglement creation. Since no notion of locality is expected in such systems, a general understanding of their dynamics is lacking. In a step towards rectifying this problem, we prove two Lieb-Robinson-type bounds that constrain the time for signaling and scrambling in strongly long-range interacting systems, for which no tight bounds were previously known. Our first bound applies to systems mappable to free-particle Hamiltonians with long-range hopping, and is saturable for ⩽ /2. Our second bound pertains to generic long-range interacting spin Hamiltonians and gives a tight lower bound for the signaling time to extensive subsets of the system for all < . This many-site signaling time lower bounds the scrambling time in strongly long-range interacting systems.
强长程相互作用量子系统——即在d维晶格上相互作用随距离以幂律1/r^α衰减(α⩽d)的系统——近年来受到了广泛关注。它们出现在量子计算和模拟的领先实验平台中,以及量子信息扰码和快速纠缠产生的理论模型中。由于在这类系统中不存在局域性的概念,因此缺乏对其动力学的全面理解。为了解决这个问题,我们证明了两个李布 - 罗宾逊型界,它们限制了强长程相互作用系统中的信号传递和扰码时间,而此前对于这类系统尚无严格的界。我们的第一个界适用于可映射到具有长程跳跃的自由粒子哈密顿量的系统,并且对于α⩽d/2是可饱和的。我们的第二个界适用于一般的长程相互作用自旋哈密顿量,并为系统的所有α<d的广泛子集给出了信号传递时间的严格下限。这个多位点信号传递时间为强长程相互作用系统中的扰码时间提供了下限。