Author Affiliations
1CAS Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei 230026, China2CAS Center for Excellence in Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei 230026, China3Institute for Quantum Control and Quantum Information and School of Physics and Materials Engineering, Hefei Normal University, Hefei 230601, Chinashow less
Fig. 1. (a) Energy diagram of the diamond configuration. (b) The schematic diagram of the experimental setup. SLM 1 and SLM 2, spatial light modulator; PBS, polarizing beam splitter; DM, long-pass dichroic mirror; SF, short-pass filter; BF, band-pass filter; BT, beam traps; SMF 1 and SMF 2, single-mode fiber; M, mirror. The focal lengths of lenses L1, L2, L3, L4, L5, and L6 are 75, 150, 150, 150, 150, and 75 mm, respectively.
Fig. 2. (a) Intensity profiles of the input POV beams (red) and the converted POV beams (blue). (b),(c) The distribution of conversion efficiency η (unit is ‰) with different values of l in the case of kr = 6.13 mm−1 and kr = 24.51 mm−1. The η is estimated from the power and wavelength of lights before and after frequency conversion.
Fig. 3. (a) Cross-talk matrix between the input and the converted beams formed by the POV states in subspace {|−6〉,…,|6〉}. (b) The theoretical, input, and converted beam intensity profiles of four 2D states. (c) The real and imaginary parts of the reconstructed density matrix for the four 2D states.
Fig. 4. (a) The theoretical, input, and converted beam intensity profiles of the 3D, 5D, and 7D states. (b) The real and imaginary parts of the reconstructed density matrix for the 3D, 5D, and 7D states. (c) The distribution of conversion efficiency η with different states |Ψ〉, where |2D1〉 = (|0〉 + |6〉)/2, |2D2〉 = (|1〉 + |−5〉)/2, |2D3〉 = (|2〉 + |4〉)/2, |2D4〉 = (|−3〉 + |−6〉)/2, |3D〉 = (|−1〉+|3〉 + |−6〉)/3, |5D〉 = (|0〉 + |1〉 + |−3〉 + |−5〉 + |6〉)/5, and |7D〉 = (|0〉 + |−1〉 + |2〉 + |3〉 + |−4〉 + |5〉 + |−6〉)/7.