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arXiv:1901.04239 · Quantum Information Processing

CNOT gate on reverse photon modes in a ring cavity

Sergey N. Andrianov, Арсланов Наркис Мусавирович, K. I. Gerasimov, Alexander A. Kalinkin, Sergey A. Moiseev

Published Jun 8, 2019• 3 citations
arXivHTMLPDF
DOI
10.1007/s11128-019-2345-z

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It is well known that a parallel quantum computer is more powerful than a classical one. So far, there are some important works about the construction of universal quantum logic gates, the key elements in quantum computation. However, they are focused on operating on one degree of freedom (DOF) of quantum systems. Here, we investigate the possibility of achieving scalable hyper-parallel quantum computation based on two DOFs of photon systems. We construct a deterministic hyper-controlled-not (hyper-CNOT) gate operating on both the spatial-mode and the polarization DOFs of a two-photon system simultaneously, by exploiting the giant optical circular birefringence induced by quantum-dot spins in double-sided optical microcavities as a result of cavity quantum electrodynamics (QED). This hyper-CNOT gate is implemented by manipulating the four qubits in the two DOFs of a two-photon system without auxiliary spatial modes or polarization modes. It reduces the operation time and the resources consumed in quantum information processing, and it is more robust against the photonic dissipation noise, compared with the integration of several cascaded CNOT gates in one DOF.
The paper discusses the gate complexity of reversible circuits with the small number of additional inputs consisting of NOT, CNOT and 2-CNOT gates. We study Shannon's gate complexity function L(n,q)L(n, q)L(n,q) for a reversible circuit implementing a Boolean transformation f ⁣:Z2n→Z2nf\colon \mathbb Z_2^n \to \mathbb Z_2^nf:Z2n​→Z2n​ with q⩽O(n2)q \leqslant O(n^2)q⩽O(n2) additional inputs. The general bound L(n,q)≍n2n/log⁡2nL(n,q) \asymp n2^n \mathop / \log_2 nL(n,q)≍n2n/log2​n is proved for this case.