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Spatial Characterization Of Two-Photon States - GAP-Optique

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3.2. OAM transfer in general SPDC configurations<br />

A special case of the lg modes is the zero-order mode that does not carry oam.<br />

Since the zero-order Laguerre polynomial L 0 0 = 1, the zero-order Laguerre-<br />

Gaussian lg00 = 1 is the Gaussian mode given by<br />

<br />

w<br />

1<br />

2<br />

LG00(q) = exp<br />

2π<br />

<br />

− w2 q 2<br />

4<br />

<br />

. (3.4)<br />

This is not, however, the only mode with oam equal to zero, the same is true<br />

for all other modes lg0p. Spiral harmonics are defined to collect all the modes<br />

with the same oam value, regardless of the value of p, these modes are defined<br />

as<br />

LGl(q) = <br />

LGlp(q) (3.5)<br />

p<br />

=al(q) exp [ilθ].<br />

The phase dependence on l, shown by each spiral harmonic mode, is exploited<br />

to determine the photon’s oam content [52]. Consider, for instance, a photon<br />

with a spatial distribution given by Φ(q), which using the spiral harmonic<br />

modes can be written as<br />

∞<br />

Φ(q) = al(q) exp [ilθ], (3.6)<br />

l=−∞<br />

so that each mode in the decomposition has a well defined oam of l per<br />

photon. Therefore, the probability Cl of having a photon with oam equal to l<br />

is the weight of the corresponding mode in the distribution:<br />

where<br />

Cl =<br />

al(q) = 1<br />

√ 2<br />

∞<br />

0<br />

2π<br />

0<br />

dq|al(q)| 2 q (3.7)<br />

dθΦ(q, θ) exp (−ilθ). (3.8)<br />

If the photon has a well defined oam of l0, the weight of the corresponding<br />

mode Cl0 = 1 and the weights of the other modes Cl=l 0 = 0. If Cl = 0 for<br />

different values of l, the photon state is a superposition of those modes with<br />

different oam values. Compared to the relative simplicity of these calculations,<br />

measuring the oam content is a more complicated task described in appendix<br />

C.<br />

Now that the techniques for the calculation of the oam content are introduced,<br />

the next section will use the spherical harmonics and the oam decomposition<br />

to study the transfer of oam from the pump photon to the signal and<br />

idler.<br />

3.2 OAM transfer in general SPDC configurations<br />

The oam carried by a photon is directly associated to its spatial shape. In<br />

order to simplify the description of the oam transfer mechanisms, this section<br />

considers only the spatial part of the mode function in a spdc configuration<br />

31

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