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The Bose-Hubbard Model is QMA-complete

机译:Bose-Hubbard模型是QMA完全的

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The Bose-Hubbard model is a system of interacting bosons that live on the vertices of a graph. The particles can move between adjacent vertices and experience a repulsive on-site interaction. The Hamil-tonian is determined by a choice of graph that specifies the geometry in which the particles move and interact. We prove that approximating the ground energy of the Bose-Hubbard model on a graph at fixed particle number is QMA-complete. In our QMA-hardness proof, we encode the history of an n-qubit computation in the subspace with at most one particle per site (i.e., hard-core bosons). This feature, along with the well-known mapping between hard-core bosons and spin systems, lets us prove a related result for a class of 2-local Hamiltonians defined by graphs that generalizes the XY model. By avoiding the use of perturba-tion theory in our analysis, we circumvent the need to multiply terms in the Hamiltonian by large coefficients.
机译:Bose-Hubbard模型是一个交互存在于图形顶点上的玻色子的系统。粒子可以在相邻的顶点之间移动,并经历排斥性的现场交互作用。 Hamiltonian是通过选择图形来确定的,该图形指定了粒子在其中移动和相互作用的几何形状。我们证明,在固定粒子数的情况下,在图上近似Bose-Hubbard模型的地面能量是QMA完全的。在我们的QMA硬度证明中,我们在每个位点最多具有一个粒子(即硬核玻色子)的子空间中对n量子位计算的历史进行编码。此功能以及硬核玻色子和自旋系统之间的众所周知的映射关系,使我们证明了由归纳XY模型的图定义的一类2局部哈密顿量的相关结果。通过在我们的分析中避免使用扰动理论,我们避免了将汉密尔顿方程中的项乘以大系数的需求。

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