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Engineering exotic phases for topologically protected quantum computation by emulating quantum dimer models

机译:通过仿真量子二聚体模型来工程化外来相,以进行受拓扑保护的量子计算

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摘要

We use a nonperturbative extended contractor renormalization (ENCORE) method for engineering quantum devices for the implementation of topologically protected quantum bits described by an effective quantum dimer model on the triangular lattice. By tuning the couplings of the device, topological protection might be achieved if the ratio between effective two-dimer interactions and flip amplitudes lies in the liquid phase of the phase diagram of the quantum dimer model. For a proposal based on a quantum Josephson junction array [L. B. Ioffe et al., Nature (London) 415, 503 (2002)] our results show that optimal operational temperatures below 1 mK can only be obtained if extra interactions and dimer flips, which are not present in the standard quantum dimer model and involve three or four dimers, are included. It is unclear if these extra terms in the quantum dimer Hamiltonian destroy the liquid phase needed for quantum computation. Minimizing the effects of multidimer terms would require energy scales in the nano-Kelvin regime. An alternative implementation based on cold atomic or molecular gases loaded into optical lattices is also discussed, and it is shown that the small energy scales involved-implying long operational times-make such a device impractical. Given the many orders of magnitude between bare couplings in devices, and the topological gap, the realization of topological phases in quantum devices requires careful engineering and large bare interaction scales.
机译:我们对工程量子设备使用非扰动扩展承包商重整化(ENCORE)方法,以实现由三角形晶格上的有效量子二聚体模型描述的受拓扑保护的量子位。通过调整设备的耦合,如果有效的二聚体相互作用和翻转幅度之间的比率位于量子二聚体模型的相图的液相中,则可以实现拓扑保护。对于基于量子约瑟夫森结阵列的建议[L. B. Ioffe et al。,Nature(London)415,503(2002)]我们的结果表明,只有在标准量子二聚体模型中不存在额外的相互作用和二聚体翻转的情况下,才能获得低于1 mK的最佳工作温度。包括三个或四个二聚体。尚不清楚量子二聚体哈密顿量中的这些额外术语是否会破坏量子计算所需的液相。最小化多二聚体项的影响将需要纳米开尔文体系中的能级。还讨论了基于加载到光学晶格中的冷原子或分子气体的另一种实现方式,并且显示出所涉及的小能量规模(意味着较长的运行时间)使这种设备不切实际。考虑到设备中裸耦合之间的数量级和拓扑间隙,量子设备中拓扑相的实现需要仔细的工程设计和较大的裸交互规模。

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