Quantum circuit mapping for universal and scalable computing in MZI-based integrated photonics

被引:3
|
作者
Kwon, Yong [1 ]
Baldazzi, Alessio [2 ]
Pavesi, Lorenzo [2 ]
Choi, Byung-Soo [3 ]
机构
[1] Pukyong Natl Univ, Dept Phys, Busan, South Korea
[2] Univ Trento, Dept Phys, Trento, Italy
[3] Pukyong Natl Univ, Dept Sci Comp, Busan, South Korea
来源
OPTICS EXPRESS | 2024年 / 32卷 / 07期
基金
欧盟地平线“2020”; 新加坡国家研究基金会;
关键词
REALIZATION; GATES;
D O I
10.1364/OE.520492
中图分类号
O43 [光学];
学科分类号
070207 ; 0803 ;
摘要
Linear optical quantum computing (LOQC) offers a quantum computation paradigm based on well -established and robust technology and flexible environmental conditions following DiVincenzo's criteria. Within this framework, integrated photonics can be utilized to achieve gate -based quantum computing, defining qubits by path -encoding, quantum gates through the use of Mach-Zehnder interferometers (MZIs), and measurements through single -photon detectors. In particular, universal two-qubit gates can be achieved by suitable structures of MZIs together with post -selection or heralding. The most resource -efficient choice is given by the post -selected Controlled -Z (CZ) gate. However, this implementation is characterized by a design which has a non -regular structure and cannot be cascaded. This limits the implementation of large-scale LOQC. Starting from these issues, we suggest an approach to move toward a universal and scalable LOQC on the integrated photonic platform. First of all, choosing the post -selected CZ as a universal two-qubit gate, we extend the path -encoded dual -rail qubit to a triplet of waveguides, composed of an auxiliary waveguide and the pair of waveguides corresponding to the qubit basis states. Additionally, we introduce a swap photonic network that maps the regularly -labeled structure of the new path -encoded qubits to the structure needed for the post -selected CZ. We also discuss the optical swap gate that allows the connection of non -nearest neighbor path -encoded qubits. In this way, we can deterministically exchange the locations of the qubits and execute controlled quantum gates between any path -encoded qubits. Next, by truncating the auxiliary waveguides after any post -selected CZ, we find that it is possible to cascade this optical gate when it acts on different pairs that share only one qubit. Finally, we show the Bell state and the Greenberger-Horne-Zeilinger (GHZ) state generation circuits implementing the regular structure, the cascading procedure of post -selected CZ and the optical swap. (c) 2024 Optica Publishing Group under the terms of the Optica Open Access Publishing Agreement
引用
收藏
页码:12852 / 12881
页数:30
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