2014
DOI: 10.1103/physreva.90.052310
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Universal hybrid three-qubit quantum gates assisted by a nitrogen-vacancy center coupled with a whispering-gallery-mode microresonator

Abstract: We investigate the construction of two universal three-qubit quantum gates in a hybrid system. The designed system consists of a flying photon and a stationary negatively charged nitrogen-vacancy (NV) center fixed on the periphery of a whispering-gallery-mode (WGM) microresonator, with the WGM cavity coupled to tapered fibers functioning as an add-drop structure. These gate operations are accomplished by encoding the information both on the spin degree of freedom of the electron confined in the NV center and o… Show more

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Cited by 37 publications
(15 citation statements)
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“…Some schemes for optical hyper-CNOT gates assisted by QDs or NV centres have been proposed by Ren et al [25][26][27]. Wang et al [28,29] designed some quantum circuits for hyper-parallel universal quantum gates acting on hybrid photon-matter systems.…”
Section: Discussion and Summarymentioning
confidence: 99%
See 1 more Smart Citation
“…Some schemes for optical hyper-CNOT gates assisted by QDs or NV centres have been proposed by Ren et al [25][26][27]. Wang et al [28,29] designed some quantum circuits for hyper-parallel universal quantum gates acting on hybrid photon-matter systems.…”
Section: Discussion and Summarymentioning
confidence: 99%
“…By the first approach, the quantum circuits for solid-state electronic CNOT gate [23] and flying photonic Toffoli gate [24] have been designed. By the second approach, schemes for implementing hyper-parallel photon-based CNOT gate [25][26][27] and hyperparallel photon-matter-based universal gates [28,29] have been proposed. The hyperentangledcluster-state-based quantum computing have been demonstrated in recent years [30].…”
Section: Introductionmentioning
confidence: 99%
“…The general resonators employed in our proposals should be polarization-degenerate ones, and they can be achieved by employing silica microtoroid resonators [64,71,76,77] fabricated on silicon wafers, H1 planar photonic crystal cavities [78][79][80][81] formed in thin semiconductor slab waveguides, micropillar cavities [82][83][84] grown by molecular-beam epitaxy on GaAs [100] substrates, or fiber-based Fabry-Perot cavities [72][73][74]. The degeneracy of the two orthogonal polarization modes of the H1 cavity is broken by systematic errors, such as hole shape and period, in the imperfect fabrication process.…”
Section: Fidelities and Efficiencies Of Our Universal Optical Quamentioning
confidence: 99%
“…Using time-dependent second-order perturbation theory applied to this perturbed oscillator, we compute the unitary evolution operator up to O(e 2 ). This approximate unitary evolution operator at time T is expressible as a linear plus a quadratic function of the electromagnetic field (E(t), B(t), 0 ≀ t ≀ T ), and hence, we are able to compute up to O(e 2 ), the error energy between this approximate unitary gate and a given unitary gate [3][4][5][6][7][8][9][10][11]. This error energy is now a linear-quadratic function of the electromagnetic field (E(t), B(t), 0 ≀ t ≀ T ).…”
Section: Introductionmentioning
confidence: 99%