2012
DOI: 10.1364/ol.37.003951
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Innovative method to investigate how the spatial correlation of the pump beam affects the purity of polarization entangled states

Abstract: We present an innovative method to address the relation between the purity of type-I polarization entangled states and the spatial properties of the pump laser beam. Our all-optical apparatus is based on a spatial light modulator, and it offers unprecedented control on the spatial phase function of the entangled states. In this way, we demonstrate quantitatively the relation between the purity of the generated state and the spatial field correlation function of the pump beam.

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Cited by 4 publications
(5 citation statements)
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References 14 publications
(21 reference statements)
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“…2, is based on PDC generated by two 1 mm adjacent type-I Beta-Barium Borate (BBO) crystals, oriented with their optical axes aligned in perpendicular planes and pumped by a 10 mW, 405 nm cw diode laser (Newport LQC405-40P). The two BBO crystals generate the signal and idler states with perpendicular polarization and the interference filter (F2) ensures a good spatial correlation between signal and idler [5,20,21]. We generate two channels 0 and 1 (corresponding to the momentum states |0 and |1 , respectively) with a double slit (DS) positioned along the idler path.…”
mentioning
confidence: 99%
“…2, is based on PDC generated by two 1 mm adjacent type-I Beta-Barium Borate (BBO) crystals, oriented with their optical axes aligned in perpendicular planes and pumped by a 10 mW, 405 nm cw diode laser (Newport LQC405-40P). The two BBO crystals generate the signal and idler states with perpendicular polarization and the interference filter (F2) ensures a good spatial correlation between signal and idler [5,20,21]. We generate two channels 0 and 1 (corresponding to the momentum states |0 and |1 , respectively) with a double slit (DS) positioned along the idler path.…”
mentioning
confidence: 99%
“…A programmable one-dimensional spatial light modulator (SLM) is placed on the path of signal and idler in order to control the visibility of the generated states. The SLM provides the setup with great flexibility, allowing the experimenter to choose and set the visibility of generated states [28,29]. Eventually, photons are focused in two multimode fibers and sent to singlephoton counting modules (CC).…”
Section: A Experimental Generation Of Werner Statesmentioning
confidence: 99%
“…Moreover, A(ω p ) is the spectral arXiv:1302.0205v2 [quant-ph] 11 Apr 2013 amplitude of the pump,F (∆k ⊥ ) is the Fourier transform of its spatial amplitude and the Sinc(∆k L/2) function arises due to the finite crystal size (L = 1mm) along the longitudinal direction. The two-crystal geometry implies that the polarization degrees of freedom of the two photons are entangled and it further introduces the phase term Φ(ω p , θ s , θ i ), which is due to the different optical paths followed by the couples of photons generated in the first and in the second crystal [27][28][29]. To first order this term reads Φ(ω p , θ s , θ i ) ≈ Φ 0 + ∆τ ω p + κθ s + ηθ i .…”
Section: The Physical System and The Experimental Apparatusmentioning
confidence: 99%
“…In fact, through the SLM we can impose an arbitrary polarization-and positiondependent phase shift to the two-photon state in Eq.(1). On the one hand, a linear phase Φ ≡ −Φ 0 − κθ s − ηθ i is set to offset the corresponding terms in the first-order expansion of Φ(ω p , θ s , θ i ) [27][28][29][30]. On the other hand, a further linear phase on both signal and idler beams emulates a time evolution of the two-photon state [31].…”
Section: The Physical System and The Experimental Apparatusmentioning
confidence: 99%
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