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arXiv 2608.29830cond-mat.supr-concond-mat.mes-hallcond-mat.stat-mech

弹道-局域化动力学作为约瑟夫森结量子相变的特征

Ballistic-to-Localized Dynamics as Signature of Quantum Phase Transition in Josephson Junction

  • Università di Napoli Federico II(那不勒斯费德里科二世大学)
  • INFN, Sezione di Napoli(意大利国家核物理研究所那不勒斯分部)
  • SPIN-CNR(凝聚态物理特殊相互作用中心研究所)
  • The Abdus Salam International Center for Theoretical Physics (ICTP)(阿卜杜斯·萨拉姆国际理论物理中心)
  • RIKEN Center for Emergent Matter Science (CEMS)(理化学研究所涌现物质科学中心)
  • Fundamental Quantum Science Program (FQSP), TRIP Headquarters, RIKEN(理化学研究所量子科学计划总部)

机构由 AI 辅助整理,请以论文原文为准。

F. G. Capone, A. de Candia, G. Di Bello, V. Cataudella, R. Fazio, N. Nagaosa, C. A. Perroni, G. De Filippis

中文总结 AI 辅助

该研究通过数值技术探究小电容约瑟夫森结在不同耗散 regime 下的行为,发现欧姆耗散强度增加会驱动 Berezinskii-Kosterlitz-Thouless 量子相变,不同耗散 regime 的相变特性存在差异,且欧姆 regime 下动力学呈弹道-局域化变化。

中文摘要 AI 辅助

我们采用最先进的数值技术,研究量子相位涨落和准粒子隧穿如何影响小电容约瑟夫森结在欧姆、亚欧姆和超欧姆耗散 regime 下的行为。我们表明,增加欧姆耗散强度会在热力学平衡中驱动 Berezinskii-Kosterlitz-Thouless 量子相变。偏离欧姆行为会深刻改变这一情况:超欧姆 regime 无相位转变,而亚欧姆 regime 呈现连续二级相变,与自旋-玻色子模型的普适类一致。在欧姆 regime 内,实频率线性响应计算显示,相位粒子不会发生通常假设的扩散-局域化交叉,相反,有限电阻会逐步抑制奇异的零频响应,产生动力学上的弹道-局域化变化。在有限频率下,与环境的耦合会在电荷响应中产生长寿命激发,随着亚间隙和分流电阻降低,该激发会演变为共振。

英文摘要

Using state-of-the-art numerical techniques, we investigate how quantum phase fluctuations and quasiparticle tunneling shape the behavior of a small-capacitance Josephson junction across Ohmic, sub-Ohmic, and super-Ohmic dissipation regimes. We show that increasing the Ohmic dissipation strength drives a Berezinskii-Kosterlitz-Thouless quantum phase transition at thermodynamic equilibrium. Deviations from Ohmic behavior profoundly alter this scenario: the super-Ohmic regime exhibits no phase transition, whereas the sub-Ohmic regime displays a continuous second-order transition, consistent with the universality classes of the spin-boson model. Within the Ohmic regime, real-frequency linear-response calculations reveal that the phase particle does not undergo the commonly assumed diffusive-to-localized crossover. Instead, finite resistance progressively suppresses the singular zero-frequency response, producing a ballistic-to-localized change in the dynamics. At finite frequencies, coupling to the environment generates a long-lived excitation in the charge response, which evolves into a resonance as the subgap and shunt resistances are reduced.

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