Decoherence in Josephson-junction qubits due to critical current fluctuations

TL;DR

This paper analyzes how critical current fluctuations cause decoherence in Josephson-junction qubits, providing a model to predict dephasing times and comparing theoretical predictions with experimental data.

Contribution

It introduces a quantitative model linking critical current noise to qubit dephasing times and compiles experimental data to validate the noise scaling across different technologies.

Findings

Dephasing time scales with critical current noise spectral density.

Critical current noise at 1 Hz scales with junction parameters.

Predicted dephasing times at 100 mK are longer than experimental values.

Abstract

We compute the decoherence caused by $1/f$ fluctuations at low frequency $f$ in the critical current $I_0$ of Josephson junctions incorporated into flux, phase, charge and hybrid flux-charge superconducting quantum bits (qubits). The dephasing time $\tau_{\phi}$ scales as $I_0/ \Omega \Lambda S_{I_0}^{1/2}(1$ Hz$)$, where $\Omega / 2\pi$ is the energy level splitting frequency, $S_{I_0}(1$ Hz$)$ is the spectral density of the critical current noise at 1 Hz, and $\Lambda \equiv |I_0 d \Omega / \Omega d I_0|$ is a parameter computed for given parameters for each type of qubit that specifies the sensitivity of the level splitting to critical current fluctuations. Computer simulations show that the envelope of the coherent oscillations of any qubit after time $t$ scales as $\exp (-t^2/ 2 \tau_{\phi}^2)$ when the dephasing due to critical current noise dominates the dephasing from all sources of dissipation. We compile published results for fluctuations in the critical current of Josephson tunnel junctions fabricated with different technologies and a wide range in $I_0$ and $A$, and show that their values of $S_{I_0}(1$ Hz$)$ scale to within a factor of three of $[ 144 (I_0/\mu{\rm A})^2/ (A/ \mu{\rm m}^2)]($pA$)^2/$Hz at 4.2 K. We empirically extrapolate $S_{I_0}^{1/2}(1$ Hz$)$ to lower temperatures using a scaling $T($K$)/4.2$. Using this result, we find that the predicted values of $\tau_{\phi}$ at 100 mK range from 0.8 to 12 $\mu$s, and are usually substantially longer than values measured experimentally at lower temperatures.