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APS -APS March Meeting 2017 - Event - Quantum simulations of a Fermi-Hubbard model using a semiconductor quantum dot array

机译:APS -APS March Meeting 2017-活动-使用半导体量子点阵列的费米-哈伯德模型的量子模拟

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Quantum dots hold a promise for quantum simulations of highly-correlated electronic phases as they readily adhere to a Fermi-Hubbard model in the elusive strong-interaction, low-temperature regime, where quantum correlations can span many sites. Working in solid-state inevitably entails disorder, however, which makes reaching homogeneity, even for small systems, rather difficult, and as such attempts at simulating Fermi-Hubbard physics in solid state have been few and far between. We describe a toolbox for semiconductor quantum dots based on interpreting well-known features in charge stability that allows for the independent tuning of site-specific energy offsets and tunnel couplings, and use this to map out the accessible parameter space of a triple quantum dot device up to a total of 12 electrons and from $t/U=0.01$ to $t/U=0.12$. As tunnel couplings are homogeneously increased, we witness the delocalization transition from Coulomb blockade to collective Coulomb blockade, a finite-size analogue of the Mott metal-to-insulator transition. A further automated application of these ideas, on larger and more homogeneous samples, will make the synthesis of tailor-made correlated-electronic phases possible in the near future.
机译:量子点为高度相关的电子相的量子模拟提供了希望,因为它们在难以捉摸的强相互作用,低温状态下易于遵循费米-哈伯德模型,在量子状态下,量子相关性可以跨越多个位置。然而,在固态下工作不可避免地会带来混乱,即使对于小型系统而言,也很难达到同质,这相当困难,因此在固态下模拟费米-哈伯德物理的尝试很少。我们基于对电荷稳定性的众所周知的特征的解释,描述了一种用于半导体量子点的工具箱,该工具箱允许对特定于站点的能量偏移和隧道耦合进行独立调整,并使用它来绘制三重量子点设备的可访问参数空间总共12个电子,从$ t / U = 0.01 $到$ t / U = 0.12 $。随着隧道耦合的均匀增加,我们看到了从库仑封锁到集体库仑封锁的离域过渡,这是莫特金属到绝缘子过渡的有限尺寸模拟。这些想法在更大和更均匀的样品上的进一步自动化应用将使在不久的将来合成定制的相关电子相成为可能。

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