# Kinetics of the superconducting charge qubit in the presence of a quasiparticle

Source: [Kinetics of the superconducting charge qubit in the presence of a quasiparticle](<https://www.sota2.com/research/paper/68fa206d7a2b558e29330f2c>)

Collection index: [llms.txt](<https://www.sota2.com/research/llms.txt>)

Data updated: 2025-10-23T21:59:17.965Z

Authors: R. M. Lutchyn, L. I. Glazman, A. I. Larkin

Published: 2006-03-24T02:09:30.000Z

## Abstract

We investigate the energy and phase relaxation of a superconducting qubit caused by a single quasiparticle. In our model, the qubit is an isolated system consisting of a small island (Cooper-pair box) and a larger superconductor (reservoir) connected with each other by a tunable Josephson junction. If such system contains an odd number of electrons, then even at lowest temperatures a single quasiparticle is present in the qubit. Tunneling of a quasiparticle between the reservoir and the Cooper-pair box results in the relaxation of the qubit. We derive master equations governing the evolution of the qubit coherences and populations. We find that the kinetics of the qubit can be characterized by two time scales - quasiparticle escape time from reservoir to the box, $\\Gamma^{-1}\_{in}$, and quasiparticle relaxation time $\\tau$. The former is determined by the dimensionless normal-state conductance $g\_T$ of the Josephson junction and one-electron level spacing $\\delta\_r$ in the reservoir ($\\Gamma\_{in}\\sim g\_T\\delta\_r$), and the latter is due to electron-phonon interaction. We find that phase coherence is damped on the time scale of $\\Gamma^{-1}\_{in}$. The qubit energy relaxation depends on the ratio of the two characteristic times, $\\tau$ and $\\Gamma^{-1}\_{in}$, and also on the ratio of temperature $T$ to the Josephson energy $E\_J$.

## Recorded benchmark results

A research result applies to its stated dataset, split, metric and evaluation configuration. Compare like-for-like settings, preserve the metric's unit and direction, and distinguish paper-reported results from independent reproduction. The best result recorded here is not a claim of exhaustive, current global coverage.

## Original sources and implementation

[Original paper](<https://arxiv.org/abs/cond-mat/0603640>)

[PDF](<https://arxiv.org/pdf/cond-mat/0603640.pdf>)
