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SINGLE-ELECTRON TRANSISTORS IN THE REGIME OF HIGH CONDUCTANCE

机译:高电导率的单电子晶体管

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We have studied high conductance single electron transistors with coupling strength up to α = 4.75. We measured the maximum and the minimum of the linear response conductance as a function of gate voltage U_g, called G_(max) and C_(min), respectively, in the temperature range from 25 mK to 18K. G_(max)(T) agrees almost perfectly with the second order perturbation theory up to α = 1.4. For larger values of α increasing deviations are observed, which have to be accounted for by more advanced techniques. The most promising approach, which has the power to describe the whole parameter range accessible to experiments, is the quantum Monte Carlo method, although the inclusion of higher orders might extend the range of validity for the perturbation theory. For G_(min) we get deviations from the second order result for all values of α investigated in this study, which is a surprising result as G_(min) is measured at a gate voltage where all charge states are far from degeneracy. Here perturbation theory does not have to deal with divergencies and is usually assumed to describe the data for moderate α. However, QMC results seem to show deviations from perturbative results similar to the ones we observe in our experiments. So also for G_(min) QMC data is the most promising candidate to describe our measurements at a quantitative level.
机译:我们已经研究了耦合强度高达α= 4.75的高电导率单电子晶体管。我们在25 mK至18K的温度范围内分别测量了线性响应电导的最大值和最小值与栅极电压U_g的关系,分别称为G_(max)和C_(min)。 G_(max)(T)与直到α= 1.4的二阶微扰理论几乎完全吻合。对于较大的α值,观察到增加的偏差,这必须通过更高级的技术来解决。最有前途的方法,它有能力描述实验可访问的整个参数范围,是量子蒙特卡洛方法,尽管包含更高的阶数可能会扩大扰动理论的有效性范围。对于G_(min),对于本研究中研究的所有α值,我们都偏离了二阶结果,这是一个令人惊讶的结果,因为G_(min)是在栅极电压下测量的,而栅极电压上的所有电荷状态都远离简并。在这里,扰动理论不必处理散度,通常假设它描述了中等α的数据。但是,QMC结果似乎显示出与微扰结果的偏差,类似于我们在实验中观察到的结果。因此,对于G_(min)QMC数据而言,最有希望在定量水平上描述我们的测量结果。

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