Pair-cat codes: autonomous error-correction with low-order nonlinearity

TL;DR

This paper introduces pair-cat codes, a two-mode bosonic system with autonomous error correction that offers exponential immunity to phase drifts and photon loss, using low-order nonlinearity and continuous monitoring.

Contribution

It presents a novel two-mode bosonic code with autonomous error correction, improved implementation features, and a generalized stabilizer formalism for multiple modes.

Findings

Exponential immunity to phase drifts in both modes.

Protection against photon loss in one mode via continuous monitoring.

Lower photon number requirement compared to cat codes.

Abstract

We introduce a driven-dissipative two-mode bosonic system whose reservoir causes simultaneous loss of two photons in each mode and whose steady states are superpositions of pair-coherent/Barut-Girardello coherent states. We show how quantum information encoded in a steady-state subspace of this system is exponentially immune to phase drifts (cavity dephasing) in both modes. Additionally, it is possible to protect information from arbitrary photon loss in either (but not simultaneously both) of the modes by continuously monitoring the difference between the expected photon numbers of the logical states. Despite employing more resources, the two-mode scheme enjoys two advantages over its one-mode cat-qubit counterpart with regards to implementation using current circuit QED technology. First, monitoring the photon number difference can be done without turning off the currently implementable dissipative stabilizing process. Second, a lower average photon number per mode is required to enjoy a level of protection at least as good as that of the cat-codes. We discuss circuit QED proposals to stabilize the code states, perform gates, and protect against photon loss via either active syndrome measurement or an autonomous procedure. We introduce quasiprobability distributions allowing us to represent two-mode states of fixed photon number difference in a two-dimensional complex plane, instead of the full four-dimensional two-mode phase space. The two-mode codes are generalized to multiple modes in an extension of the stabilizer formalism to non-diagonalizable stabilizers. The $M$-mode codes can protect against either arbitrary photon losses in up to $M-1$ modes or arbitrary losses and gains in any one mode.