1.Centre for Quantum Computation and Communication Technology, Department of Quantum Science, The Australian National University, Canberra, Australia
2.Centre for Engineered Quantum Systems, Department of Physics & Astronomy, Macquarie University, North Ryde NSW 2109, Australia
Professor PK Lam, Centre for Quantum Computation and Communication Technology, Department of Quantum Science, Bld 38A, The Australian National University, Canberra ACT 0200, Australia. E-mail: Ping.Lam@anu.edu.au
纸质出版日期:2012-03,
网络出版日期:2012-12-07,
收稿日期:2012-05-09,
修回日期:2012-07-12,
录用日期:2012-07-16
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Memory-enhanced noiseless cross-phase modulation[J]. LSA, 2012,1(1).
Hosseini, M. et al. Memory-enhanced noiseless cross-phase modulation. Light: Science & Applications, 1, e40 (2012).
Memory-enhanced noiseless cross-phase modulation[J]. LSA, 2012,1(1). DOI: 10.1038/lsa.2012.40.
Hosseini, M. et al. Memory-enhanced noiseless cross-phase modulation. Light: Science & Applications, 1, e40 (2012). DOI: 10.1038/lsa.2012.40.
Large nonlinearity at the single-photon level can pave the way for the implementation of universal quantum gates. However
realizing large and noiseless nonlinearity at such low light levels has been a great challenge for scientists in the past decade. Here
we propose a scheme that enables substantial nonlinear interaction between two light fields that are both stored in an atomic memory. Semiclassical and quantum simulations demonstrate the feasibility of achieving large cross-phase modulation (XPM) down to the single-photon level. The proposed scheme can be used to implement parity gates from which CNOT gates can be constructed. Furthermore
we present a proof of principle experimental demonstration of XPM between two optical pulses: one stored and one freely propagating through the memory medium.
CNOT gatecross-phase modulationelectromagnetically induced transparencyparity gatequantum memory
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