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arXiv 0812.2368quant-phcond-mat.stat-mech
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经典自旋模型的完备性与普适量子计算

Completeness of classical spin models and universal quantum computation

Gemma De las Cuevas, Wolfgang Dür, Maarten Van den Nest, Hans J. Briegel

摘要:

我们研究不同的经典自旋系统之间的映射,离开配分函数不变。如最近在[物理学。100,110501(2008)],在存在非均匀磁场的情况下的2D正方形晶格伊辛模型的配分函数,可以专用于任意图上的任何伊辛系统的配分函数。在这个意义上,二维伊辛模型被称为“完整的”。然而,为了获得上述结果,2D晶格上的耦合强度必须假定为复数值,因此不允许物理解释。在这里,我们将展示如何一个完整的模型与真正的-因此,“物理”-耦合可以得到,如果考虑三维伊辛模型。我们还展示了如何将一般的q态系统与可能的多体相互作用映射到具有复参数的二维伊辛模型,并给出了这些模型的完备性结果。我们还表明,在这些建设的计算开销是在所有相关的情况下多项式。这些结果证明了调用最近发现的交叉连接之间的统计力学和量子信息理论,其中配分函数表示为量子力学振幅。在这个框架内,多体量子态和完整的经典自旋系统之间存在着自然的对应关系,这些量子态允许仅通过局部测量进行通用量子计算。

英文摘要:

We study mappings between distinct classical spin systems that leave the partition function invariant. As recently shown in [Phys. Rev. Lett. 100, 110501 (2008)], the partition function of the 2D square lattice Ising model in the presence of an inhomogeneous magnetic field, can specialize to the partition function of any Ising system on an arbitrary graph. In this sense the 2D Ising model is said to be "complete". However, in order to obtain the above result, the coupling strengths on the 2D lattice must assume complex values, and thus do not allow for a physical interpretation. Here we show how a complete model with real -and, hence, "physical"- couplings can be obtained if the 3D Ising model is considered. We furthermore show how to map general q-state systems with possibly many-body interactions to the 2D Ising model with complex parameters, and give completeness results for these models with real parameters. We also demonstrate that the computational overhead in these constructions is in all relevant cases polynomial. These results are proved by invoking a recently found cross-connection between statistical mechanics and quantum information theory, where partition functions are expressed as quantum mechanical amplitudes. Within this framework, there exists a natural correspondence between many-body quantum states that allow universal quantum computation via local measurements only, and complete classical spin systems.

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