2014
DOI: 10.1038/srep05732
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Parallel Photonic Quantum Computation Assisted by Quantum Dots in One-Side Optical Microcavities

Abstract: Universal quantum logic gates are important elements for a quantum computer. In contrast to previous constructions on one degree of freedom (DOF) of quantum systems, we investigate the possibility of parallel quantum computations dependent on two DOFs of photon systems. We construct deterministic hyper-controlled-not (hyper-CNOT) gates operating on the spatial-mode and the polarization DOFs of two-photon or one-photon systems by exploring the giant optical circular birefringence induced by quantum-dot spins in… Show more

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Cited by 34 publications
(46 citation statements)
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“…Assisted by single photon or single spin gate operations, these gates can be converted to the popular quantum gates in different systems, e.g., controlled-NOT (CNOT) or hyper CNOT gates, Toffoli gates, and Fredkin gates which can be useful for scalable quantum computing73747576. Similar quantum gates, i.e., the controlled phase-flip gates were proposed by Duan and Kimble60 in atom-cavity systems have been experimentally demonstrated recently4950.…”
Section: Resultsmentioning
confidence: 94%
“…Assisted by single photon or single spin gate operations, these gates can be converted to the popular quantum gates in different systems, e.g., controlled-NOT (CNOT) or hyper CNOT gates, Toffoli gates, and Fredkin gates which can be useful for scalable quantum computing73747576. Similar quantum gates, i.e., the controlled phase-flip gates were proposed by Duan and Kimble60 in atom-cavity systems have been experimentally demonstrated recently4950.…”
Section: Resultsmentioning
confidence: 94%
“…With these interactions, several hybrid quantum logic gates may be achieved [48][49][50][51][52][53][54][55].…”
Section: Photon-atom Interaction In Optical Microcavitiesmentioning
confidence: 99%
“…Conversely, if the excess electron spin is in the state | ↓ , after reflection the pulse |R gets a phase shift of θ h while the pulse |L gets a phase shift of θ 0 . Generally, for initial electron spin in the state α 2 | ↑ + β 2 | ↓ , the optical interaction leads to the following transformation [32,40,50,52]:…”
Section: Cavity-qed Systemmentioning
confidence: 99%
“…By adjusting the frequencies c → 0, the phase difference θ 0 − θ f = π is followed for the strong coupling g κ, γ . Thus the dynamics of the interaction between photon and electron spin in a microcavity coupled system [40,52] is described as follows:…”
Section: Cavity-qed Systemmentioning
confidence: 99%