Abstract
The coherent-state qubit is a promising candidate for optical quantum information processing due to its nearly-deterministic nature of the Bell-state measurement (BSM). However, its non-orthogonality incurs difficulties such as failure of the BSM. One may use a large amplitude ($\alpha$) for the coherent state to minimize the failure probability, but the qubit then becomes more vulnerable to dephasing by photon loss. We propose a hardware-efficient concatenated BSM (CBSM) scheme with modified parity encoding using coherent states with reasonably small amplitudes ($|\alpha| \lessapprox 2$), which simultaneously suppresses both failures and dephasing in the BSM procedure. We numerically show that the CBSM scheme achieves a success probability arbitrarily close to unity for appropriate values of $\alpha$ and sufficiently low photon loss rates (e.g., $\lessapprox 5\%$). Furthermore, we verify that the quantum repeater scheme exploiting the CBSM scheme for quantum error correction enables one to carry out efficient long-range quantum communication over 1000 km. We show that the performance is comparable to those of other up-to-date methods or even outperforms them for some cases. Finally, we present methods to prepare logical qubits under modified parity encoding and implement elementary logical operations, which consist of several physical-level ingredients such as generation of Schr\"odinger's cat state and elementary gates under coherent-state basis. Our work demonstrates that the encoded coherent-state qubits in free-propagating fields provide an alternative route to fault-tolerant information processing, especially long-range quantum communication.
Highlights
Optical systems are a competitive candidate for quantum information processing (QIP) due to their long coherence time and advantages in long-distance transmission [1]
We present a hardware-efficient scheme that can significantly reduce the expected cost of the concatenated Bell-state measurement (CBSM) defined in terms of the expected number of physicallevel Bell-state measurement (BSM) used for a single CBSM
Note that there are four free parameters related to the hardware-efficient CBSM scheme: n, m, α, and j. n and m determine the block- and physical-level repetition sizes of the scheme, respectively. α is the amplitude of the coherent state constituting the logical basis. j is the letter solidity parameter, which is the number of not-failed blocks used for the majority vote of letters in the logical level
Summary
Optical systems are a competitive candidate for quantum information processing (QIP) due to their long coherence time and advantages in long-distance transmission [1]. It was claimed that a simple one-dimensional (1D) repetition cat code enables hardware-efficient topologically protected quantum computation by exploiting the 2D phase space for logical operations [43] These studies mainly deal with coherent-state qubits inside a cavity system, and they cannot be directly applied to fault-tolerant QIP in free-propagating optical fields. In this paper, motivated by recent works on the concatenated Bell-state measurement (CBSM) with multiphoton polarization qubits [11,44] and the repetition cat code [43], we overcome these obstacles by introducing the CBSM with the modified parity encoding employing coherent states.
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