Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Il Nuovo cimento della Società italiana di fisica. B/Il Nuovo cimento B

A note on tunnelling with friction

M. Kraev

Published Nov 1, 1988• 0 citations
Publisher
DOI
10.1007/bf02728787

Related papers

No friction, no tunnelling

Thomas Pilgerstorfer, Nedim Radončić

•Jan 1, 2010•1 citation

A note on the tunneling time problem

Francis E. Low, Paul F. Mende

Annals of Physics•Sep 1, 1991•61 citations

Notes on the tunneling time and trajectory

Anedio Ranfagni, Daniela Mugnai

•Jan 1, 1988•0 citations

A note on traversal time for tunneling

A. M. Jayannavar

Pramana•Oct 1, 1987•13 citations

On tunnelling with dissipation

P. Fr�brich, R. Lipperheide, K. M�hring

The European Physical Journal B•Jun 1, 1990•14 citations

Friction in macroscopic tunneling

V. P. Krainov

Abstract Macroscopic tunneling of Cooper pairs of electrons in a system of two superconductors separated by an insulator was modeled by Caldeira and Leggett by quantum-mechanical motion of a particle through the potential barrier. Friction (conductivity of the Josephson contact in experiments) was modeled by a one-dimensional phonon thermostat that interacts with the particle. Then the tunneling exponent was expressed in terms of the friction coefficient determined by the thermostat parameters. Alternatively, we propose a direct introduction of the friction coefficient into a classical action in the tunneling exponent using the method of imaginary time. As a result, the numerical coefficient of the classical friction contribution to the tunneling exponent is obtained.

Theoretical and Mathematical Physics•Apr 1, 2026•0 citations
Abstract Macroscopic tunneling of Cooper pairs of electrons in a system of two superconductors separated by an insulator was modeled by Caldeira and Leggett by quantum-mechanical motion of a particle through the potential barrier. Friction (conductivity of the Josephson contact in experiments) was modeled by a one-dimensional phonon thermostat that interacts with the particle. Then the tunneling exponent was expressed in terms of the friction coefficient determined by the thermostat parameters. Alternatively, we propose a direct introduction of the friction coefficient into a classical action in the tunneling exponent using the method of imaginary time. As a result, the numerical coefficient of the classical friction contribution to the tunneling exponent is obtained.