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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 liveon the vertices of a graph. The particles can move between adjacentvertices and experience a repulsive on-site interaction. TheHamiltonian is determined by a choice of graph that specifies thegeometry in which the particles move and interact. We prove thatapproximating the ground energy of the Bose-Hubbard model on a graphat fixed particle number is QMA-complete. In our QMA-hardness proof,we encode the history of an $n$-qubit computation in the subspace withat most one particle per site (i.e., hard-core bosons). This feature,along with the well-known mapping between hard-core bosons and spinsystems, lets us prove a related result for a class of $2$-localHamiltonians defined by graphs that generalizes the XY model. Byavoiding the use of perturbation theory in our analysis, we circumventthe need to multiply terms in the Hamiltonian by large coefficients.
机译:Bose-Hubbard模型是一个交互玻色子的系统,该玻色子位于图形的顶点上。粒子可以在相邻顶点之间移动,并经历排斥性的现场交互。哈密​​顿量是通过选择图形来确定的,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,在固定粒子数的图形上近似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包含一个粒子(即硬核玻色子)的子空间中编码$ n $ -qubit计算的历史记录。此功能以及众所周知的硬核玻色子与自旋系统之间的映射关系,使我们证明了由广义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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