Dynamically Generated Logical Qubits
Matthew B. Hastings,Jeongwan Haah +1 more
- 19 Oct 2021
- Vol. 5, pp 564
TL;DR: In this article, a quantum error correcting code with dynamically generated logical qubits is presented, which allows the code to act as a fault-tolerant quantum memory, but it does not have a logical qubit.
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Abstract: We present a quantum error correcting code with dynamically generated logical qubits. When viewed as a subsystem code, the code has no logical qubits. Nevertheless, our measurement patterns generate logical qubits, allowing the code to act as a fault-tolerant quantum memory. Our particular code gives a model very similar to the two-dimensional toric code, but each measurement is a two-qubit Pauli measurement.
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Stabilizer formalism for operator quantum error correction
TL;DR: This Letter identifies a gauge symmetry in Shor's 9-qubit code that allows us to remove 3 of its 8 stabilizer generators, leading to a simpler decoding procedure and a wider class of logical operations without affecting its essential properties, which opens the path to possible improvements of the error threshold of fault-tolerant quantum computing.
Dynamical purification phase transitions induced by quantum measurements
Michael Gullans,David A. Huse +1 more
TL;DR: In this paper, it was shown that, for mixed initial states, a balanced competition between measurements and entangling interactions within the system can result in a dynamical purification phase transition between (i) a phase that locally purifies at a constant system-size independent rate, and (ii) a "mixed" phase where the purification time diverges exponentially in the system size.
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Topological subsystem codes
TL;DR: A general mapping connecting suitable classical statistical mechanical models to optimal error correction in subsystem stabilizer codes that suffer from depolarizing noise is given.
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Subsystem surface codes with three-qubit check operators
TL;DR: In this article, a simplified version of the Kitaev's surface code was proposed, in which error correction requires only three-qubit parity measurements for Pauli operators XXX and ZZZ.
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