Measurement-based fault-tolerant architecture for quibbler code

By employing quantum error correction technology based on "four-legged cat code," and utilizing the dispersion coupling and measurement interaction between auxiliary qubits and logical qubits, fault-tolerant operations on boson systems in quantum information processing systems are achieved. This solves the problems of quantum state decoherence and auxiliary qubit errors, thereby improving the robustness of quantum computing.

CN118575070B9Active Publication Date: 2025-12-30YALE UNIVERSITY
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Patent Information

Application Number
CN202280089391.1
Authority / Receiving Office
CN · China
Patent Type
Patents(China)
Current Assignee / Owner
Priority Date
2021-12-22
Filing Date
2022-12-22
Publication Date
2025-12-30
Estimated Expiration
2042-12-22

AI Technical Summary

Technical Problem

In existing quantum information processing systems, the quantum states of boson systems are susceptible to decoherence and other noise, leading to information loss. Furthermore, traditional error correction methods cannot effectively correct errors introduced by auxiliary qubits.

Method used

The quantum error correction technology using four-legged cat code achieves non-destructive and fault-tolerant measurement of Z, ZZ, and ZZZ logical operators by using dispersion-coupled auxiliary qubits and logic qubits and the interaction of measurement and beam splitters. Combined with cavity displacement operations, it performs parity operations and error correction, including fault-tolerant SNAP gates and teleportation schemes.

Benefits of technology

It effectively corrects errors in the boson system, improves the stability of quantum states and the reliability of information storage, realizes fault-tolerant operations for quantum computing, and enhances the robustness of quantum computing.

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Abstract

Systems and methods for performing fault-tolerant quantum operations for cat code are provided. A quantum system includes an ancilla qubit dispersively coupled to a first logical qubit, and the quantum system can be operated at least in part by: generating a first drive waveform and applying the first drive waveform to the ancilla qubit, the first drive waveform including a first comb of pi pulses having selective frequencies corresponding to a first selected pair of even and odd cavity resonance frequencies of the first logical qubit; and reading out a state of the ancilla qubit.
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