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Nonequilibrium finite-frequency noise of a resonance-level quantum dot close to a dissipative quantum phase transition: Functional Renormalization Group approaches

机译:共振能量子点的非平衡有限频率噪声   接近耗散量子相变:功能重整化   小组方法

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摘要

We calculate the finite-frequency current noise of a nonequilibriumresonance-level quantum dot close to a dissipative quantum phase transition ofthe Kosterlitz-Thouless (KT) type between a de-localized phase for weakdissipation and a localized phase for strong dissipation. The resonance-levelis coupled to two spinless fermionic baths with a finite bias voltage and anOhmic boson bath representing the dissipative environment. The system isequivalent to an effective anisotropic Kondo model out of equilibrium. Tocompute the finite-frequency noise, we combine two recently developedFunctional Renormalization Group (FRG) approaches in Refs.[17,22] and inRef.[23]. The nonequilibrium current noise at zero-temperature and finitefrequencies shows a singular dip in the de-localized phase for the magnitude offrequencies equal to the bias voltage; while the dip is smeared out as thesystem moves to the localized phase. The corresponding peak-to-dip crossover isfound in the AC conductance for the magnitude of frequencies equal to the biasvoltage. The relevance and applications of our results for the experiments andfor tunnelings between Fractional Quantum Hall Edge (FQHE) states and chiralLuttinger liquids are discussed.
机译:我们计算了非平衡共振水平量子点的有限频率电流噪声,该量子点接近于Kosterlitz-Thouless(KT)类型的耗散量子相变之间的弱耗散的非定域相位与强耗散的局部相之间。共振能级耦合到两个具有有限偏置电压的无纺铁磁浴和一个代表耗散环境的欧姆玻色子浴。该系统等效于不平衡的有效各向异性近藤模型。为了计算有限频率噪声,我们在参考文献[17,22]和inRef。[23]中结合了两种最新开发的功能重整化组(FRG)方法。在零温度和有限频率下的非平衡电流噪声在离域相位中出现奇异的下降,因为频率的大小等于偏置电压。当系统移向本地化阶段时,浸入被抹去。在交流电导中发现了对应于偏置电压的频率幅度的相应峰峰间跨度。讨论了我们的结果对于实验和分数量子霍尔边缘(FQHE)态与手性Luttinger液体之间的隧穿的相关性和应用。

著录项

  • 作者

    Chung, Chung-Hou;

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  • 年度 2012
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  • 原文格式 PDF
  • 正文语种 {"code":"en","name":"English","id":9}
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