Spectral-hole memory for light at the single-photon level

被引:9
|
作者
Kutluer, Kutlu [1 ]
Florencia Pascual-Winter, Maria [2 ,3 ]
Dajczgewand, Julian [4 ,5 ]
Ledingham, Patrick M. [1 ,7 ]
Mazzera, Margherita [1 ]
Chaneliere, Thierry [4 ,5 ]
de Riedmatten, Hugues [1 ,6 ]
机构
[1] Barcelona Inst Technol, ICFO Inst Ciencies Foton, Mediterranean Technol Pk, Barcelona 08860, Spain
[2] CNEA, Ctr Atom Bariloche, Lab Foton & Optoelect, RA-8400 San Carlos De Bariloche, Rio Negro, Argentina
[3] CNEA, Inst Balseiro, RA-8400 San Carlos De Bariloche, Rio Negro, Argentina
[4] Univ Paris 11, CNRS, Lab Aime Cotton UMR 9188, Batiment 505,Campus Univ, F-91405 Orsay, France
[5] ENS Cachan, Batiment 505,Campus Univ, F-91405 Orsay, France
[6] ICREA, Barcelona 08015, Spain
[7] Univ Oxford, Clarendon Lab, Parks Rd, Oxford OX1 3PU, England
关键词
ATOMIC ENSEMBLES; QUANTUM MEMORY; LINEAR OPTICS; ULTRASLOW LIGHT; STORAGE; ENTANGLEMENT; RETRIEVAL; INTERFACE;
D O I
10.1103/PhysRevA.93.040302
中图分类号
O43 [光学];
学科分类号
070207 ; 0803 ;
摘要
We demonstrate a solid-state spin-wave optical memory based on stopped light in a spectral hole. A long-lived narrow spectral hole is created by optical pumping in the inhomogeneous absorption profile of a Pr3+ : Y2SiO5 crystal. Optical pulses sent through the spectral hole experience a strong reduction of their group velocity and are spatially compressed in the crystal. A short Raman pulse transfers the optical excitation to the spin state before the light pulse exits the crystal, effectively stopping the light. After a controllable delay, a second Raman pulse is sent, which leads to the emission of the stored photons. We reach storage and retrieval efficiencies for bright pulses of up to 39% in a 5-mm-long crystal. We also show that our device works at the single-photon level by storing and retrieving 3-mu s-long weak coherent pulses with efficiencies up to 31%, demonstrating the most efficient spin-wave solid-state optical memory at the single-photon level so far. We reach an unconditional noise level of (9 +/- 1) x 10(-3) photons per pulse in a detection window of 4 mu s, leading to a signal-to-noise ratio of 33 +/- 4 for an average input photon number of 1, making our device promising for long-lived storage of nonclassical light.
引用
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页数:5
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