Spatial Characterization Of Two-Photon States - GAP-Optique
Spatial Characterization Of Two-Photon States - GAP-Optique
Spatial Characterization Of Two-Photon States - GAP-Optique
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CHAPTER 6<br />
Summary<br />
This thesis characterizes the correlations in two-photon quantum states, both<br />
between photons, and between the spatial and frequency degrees of freedom.<br />
The photon pairs are generated by spontaneous parametric down-conversion<br />
spdc, or by the excitation of Raman transitions in cold atomic ensembles.<br />
Special attention is given to the entanglement of the photon pair in the spatial<br />
degree of freedom, associated to the orbital angular momentum oam. The<br />
main contributions or the thesis are:<br />
A novel matrix formalism to describe the two-photon mode function.<br />
This formalism makes it possible to analytically calculate several features<br />
of the down-converted photons, and reduces the numerical calculation time of<br />
other features, as shown in chapter 1 and reference [41].<br />
Analytical expressions for the purity of the subsystems formed by<br />
a single photon in space and frequency, or by a spatial two-photon<br />
state. These expressions quantify the correlations in the two-photon state,<br />
and make the effect of the various parameters of the spdc process on these<br />
correlations explicit. The thesis presents a set of conditions to suppress or<br />
enhance the correlations between the photons, or between degrees of freedom<br />
in the two-photon state. With these conditions, it is possible to design spdc<br />
sources with specific levels of correlations, for example, sources that generate<br />
pure heralded single photons, or alternatively, maximally entangled states; as<br />
shown in chapter 2 and in references [41, 45].<br />
A selection rule for oam transfer. This selection rule explains several<br />
contradictory measurements of the oam transfer from the pump beam to the<br />
signal and idler photons in spdc. We showed that the oam content of the<br />
pump is completely transferred to the photons emitted in all directions. This<br />
selection rule always holds if all possible emission directions are considered,<br />
for example in collinear configurations, but not necessarily if only a part of<br />
all emission directions is detected. These conditions for the validity of the<br />
selection rule give clear guidelines for the design of sources for protocols that<br />
exploit the multidimensionality of oam, as shown in chapter 3 and references<br />
[71, 72].<br />
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