Spatial Characterization Of Two-Photon States - GAP-Optique
Spatial Characterization Of Two-Photon States - GAP-Optique Spatial Characterization Of Two-Photon States - GAP-Optique
4. OAM transfer in noncollinear configurations The different spatial shapes in figure 4.12 clearly show that the downconversion cone does not posses azimuthal symmetry. As was predicted by the theoretical calculations, the coincidence measurement for α = 90 ◦ , presents a nearly Gaussian shape, while the other cases are highly elliptical. The slight discrepancies between experimental data and theoretical predictions observed might be due to the small (but not negligible) bandwidth of the pump beam, and due to the fact that the resolution of our system is limited by the detection pinhole size. Conclusion The spdc parameters and the detection system determine the portion of the cone that is detected in a noncollinear configuration. This chapter explains how the pump beam waist and the Poynting vector walk-off affect the oam transfer. By tailoring both parameters it is possible to generate photons with specific spatial shapes. The walk-off affects especially those configurations where pairs of photons with different α are used. The next chapter extends the analysis of the spatial correlations to pairs of photons generated in Raman transitions. The chapter describes how the specific characteristics of that source are translated into the two-photon spatial state. 50
CHAPTER 5 Spatial correlations in Raman transitions Two-photon states can be generated in different nonlinear processes, and in every case the oam transfer will depend on the particular configuration. Raman transition is an alternative method for the generation of two-photon states. Several authors have proven the generation of correlated photons in polarization [59], frequency [60] and oam [23] via Raman transitions. Typical configurations involve the partial detection of the generated photons [61, 62, 63] in quasi-collinear configurations [64]. Just as in the case of spdc, the geometrical conditions determine the oam transfer. This chapter analyses the oam transfer in Raman transitions using the techniques of the previous chapters. This chapter is divided in three sections. Section 5.1 describes the generated two-photon state by introducing its mode function. Section 5.2 studies the oam content of one of the photons with the oam of the other photons fixed. Section 5.3 describes the effect of the geometry of the process on the spatial entanglement between the photons. Numerical calculations show the effect of the geometrical configuration on the oam transfer mechanism. The finite size of the nonlinear medium results in new effects that do not appear in spdc. 51
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4. OAM transfer in noncollinear configurations<br />
The different spatial shapes in figure 4.12 clearly show that the downconversion<br />
cone does not posses azimuthal symmetry. As was predicted by the<br />
theoretical calculations, the coincidence measurement for α = 90 ◦ , presents a<br />
nearly Gaussian shape, while the other cases are highly elliptical.<br />
The slight discrepancies between experimental data and theoretical predictions<br />
observed might be due to the small (but not negligible) bandwidth of the<br />
pump beam, and due to the fact that the resolution of our system is limited<br />
by the detection pinhole size.<br />
Conclusion<br />
The spdc parameters and the detection system determine the portion of the<br />
cone that is detected in a noncollinear configuration. This chapter explains how<br />
the pump beam waist and the Poynting vector walk-off affect the oam transfer.<br />
By tailoring both parameters it is possible to generate photons with specific<br />
spatial shapes. The walk-off affects especially those configurations where pairs<br />
of photons with different α are used.<br />
The next chapter extends the analysis of the spatial correlations to pairs<br />
of photons generated in Raman transitions. The chapter describes how the<br />
specific characteristics of that source are translated into the two-photon spatial<br />
state.<br />
50