Sep 20 – 25, 2026
University of Graz
Europe/Vienna timezone

The Schmid transition in resistively shunted Josephson junction: BKT universality and transport properties

Sep 22, 2026, 10:30 AM
30m
HS 15.13 (University of Graz)

HS 15.13

University of Graz

15 - RESOWI E, 1st floor
4) Invited talk M10 - Mesoscopic superconductivity and quantum circuits Mini-Colloquium

Speaker

Francesco Giuseppe Capone (Dipartimento di Fisica "Ettore Pancini", Università degli Studi di Napoli Federico II - INFN, sezione di Napoli)

Description

The Schmid transition represents a fundamental insulator-to-superconductor phase transition occurring in the resistively shunted Josephson junction (RSJJ). The system is modeled as a parallel circuit with a non-linear inductor (Josephson energy $E_J$), a capacitor (charging energy $E_C = 4e^2/2C$), and a shunt resistor $R_S$. Initially, Schmid and Bulgadaev [1,2] predicted this transition at $\alpha = R_q/R_S = 1$, with $R_q = h/4e^2$ being the resistance quantum. Nevertheless, recent theoretical [3,4] and experimental [5] studies have challenged its existence, reviving the debate on its transport implications. In this work, we clarify the transition's nature by introducing a distinct binary order parameter $S$. We establish that it falls into the Berezinskii-Kosterlitz-Thouless (BKT) universality class [6,7], evidenced by the logarithmic decay of correlation functions near the critical point. Employing linear response theory, we show the transition's hallmark is the weight of the delta function $D_Q$ at $\omega = 0$ in the resistive response function $\Psi_{\text{reg},Q}(\omega)$ [6]. Remarkably, it lacks a low-frequency Drude peak, demonstrating that dissipation is avoided even in the insulating phase. An out-of-equilibrium analysis under small injected currents further confirms this non-dissipative dynamics.

References
[1] A. Schmid, "Diffusion and Localization in a Dissipative Quantum System", Phys. Rev. Lett. 51, 1506 (1983).
[2] S. Bulgadaev, "Phase diagram of a dissipative quantum system", ZhETF Pisma Redaktsiiu 39, 315 (1984).
[3] K. Masuki, H. Sudo, M. Oshikawa, and Y. Ashida, "Absence versus Presence of Dissipative Quantum Phase Transition in Josephson Junctions", Phys. Rev. Lett. 129, 087001 (2022).
[4] C. Altimiras, D. Esteve, C¸ . Girit, H. Le Sueur, and P. Joyez, "Absence of a dissipative quantum phase transition in Josephson junctions: Theory" arXiv:2312.14754, (2023).
[5] A. Murani, N. Bourlet, H. le Sueur, F. Portier, C. Altimiras, D. Esteve, H. Grabert, J. Stockburger, J. Ankerhold, and P. Joyez, "Absence of a dissipative quantum phase transition in Josephson junction", Phys. Rev. X 11, 018002 (2021).
[6] F. G. Capone, A. de Candia, V. Cataudella, N. Nagaosa, C. A. Perroni, and G. De Filippis, "A Clue on Small-Capacitance Josephson Junction: What to Expect from Cooper Pair Ideal Conductor and Ohmic Resistor in Parallel?", arXiv:2504.00258, (2025).
[7] F. G. Capone, A. de Candia, V. Cataudella, R. Fazio, N. Nagaosa, C. A. Perroni, and G. De Filippis "Quantum Brownian Motion: proving that the Schmid transition belongs to the Berezinskii-Kosterlitz-Thouless universality class", arXiv:2603.16227, (2025).

Author

Francesco Giuseppe Capone (Dipartimento di Fisica "Ettore Pancini", Università degli Studi di Napoli Federico II - INFN, sezione di Napoli)

Co-authors

Antonio De Candia (Università degli Studi di Napoli Federico II) Vittorio Cataudella (Università degli Studi di Napoli Federico II) Prof. Rosario Fazio (The Abdus Salam International Center for Theoretical Physics (ICTP), Strada Costiera 11, 34151 Trieste, Italy) Naoto Nagaosa Carmine Antonio Perroni (Università degli Studi di Napoli Federico II) Giulio De Filippis (Università degli Studi di Napoli Federico II)

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