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Consequences of Many-Cell Correlations in Clocked Quantum-Dot Cellular Automata

机译:时钟量子点细胞自动机中多细胞相关性的后果。

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Quantum-dot cellular automata (QCA) provides a basis for classical computation without transistors. Many simulations of QCA rely upon the so-called intercellular Hartree approximation (ICHA), which neglects the possibility of entanglement between cells. The ICHA was originally proposed as a solution to the problem of exponential scaling in the computational cost of fully quantum mechanical treatments. However, in some cases, the ICHA predicted errors in QCA operation, and quantum correlations were required for circuits to operate correctly. While quantum correlations can remedy certain problems that present themselves in ICHA calculations, here we present simulations that show that quantum correlations may in fact be problematic in other situations, such as clocked QCA. Small groups of QCA cells are modelled with a Hamiltonian analogous to a quantum mechanical Ising-like spin chain in a transverse field, including the effects of intercellular entanglement completely. When energy relaxation is included in the model, we find that intercellular entanglement changes the qualitative behavior of the system, and new features appear. In clocked QCA, isolated groups of active cells have a tendency to oscillate between polarization states as information propagates. Additionally, energy relaxation tends to bring groups of cells to an unpolarized steady state. This contrasts with the results of previous simulations, which employed the ICHA. The ICHA may in fact be a good approximation in the limit of very low tunneling rates, which can be realized in lithographically defined quantum dots. However, in molecular and atomic implementations of QCA, entanglement will play a greater role. The degree to which intercellular correlations pose a problem for memory, and clocking depends upon implementation-specific details of the interaction of the system with its environment, as well as the system's internal dynamics.
机译:量子点元胞自动机(QCA)为没有晶体管的经典计算提供了基础。 QCA的许多模拟都依赖于所谓的细胞间Hartree近似(ICHA),它忽略了细胞之间纠缠的可能性。最初提出ICHA是为了解决全量子力学处理的计算成本中的指数缩放问题。但是,在某些情况下,ICHA会预测QCA操作中的错误,并且需要量子相关性才能使电路正确运行。虽然量子相关性可以弥补ICHA计算中出现的某些问题,但在此我们提供的模拟结果表明,量子相关性实际上在其他情况下可能会出现问题,例如时钟QCA。使用汉密尔顿模型模拟一小组QCA细胞,该分子类似于横向场中的量子力学类Ising类自旋链,包括完全的细胞间纠缠效应。当模型中包含能量弛豫时,我们发现细胞间纠缠改变了系统的定性行为,并出现了新的特征。在时钟控制的QCA中,隔离的活动单元组具有随着信息传播而在极化状态之间振荡的趋势。另外,能量松弛趋向于使细胞群进入非极化的稳态。这与以前采用ICHA的模拟结果相反。实际上,在非常低的隧穿速率的极限中,ICHA可能是一个很好的近似值,这可以在光刻定义的量子点中实现。但是,在QCA的分子和原子实现中,纠缠将发挥更大的作用。细胞间相关性对内存造成问题的程度以及时钟取决于系统与环境之间相互作用的特定于实现的细节以及系统的内部动态。

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