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Spatial Characterization Of Two-Photon States - GAP-Optique

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v =γ 2 L 2 Np sin ϕi − γ 2 L 2 Ns cos ϕs sin ϕi − w 2 pNs sin ϕs cos ϕi<br />

+ γ 2 L 2 Np cos ϕi tan ρ0 sin α − γ 2 L 2 Ns cos ϕs cos ϕi tan ρ0 sin α<br />

− γ 2 L 2 Ns sin ϕs sin ϕi tan ρ0 sin α − γ 2 L 2 Ns cos ϕi sin ϕs tan ρ0 2 sin α 2<br />

w =γ 2 L 2 Np sin ϕi − γ 2 L 2 Ni sin ϕi cos ϕi + w 2 pNi sin ϕi cos ϕi<br />

+ γ 2 L 2 Np cos ϕi tan ρ0 sin α − γ 2 L 2 Ni cos ϕi 2 tan ρ0 sin α<br />

+ γ 2 L 2 Ni sin ϕi 2 tan ρ0 sin α + γ 2 L 2 Ni sin ϕi cos ϕi tan ρ0 2 sin α 2<br />

z =γ 2 L 2 N 2 p − γ 2 L 2 NpNi cos ϕi − γ 2 L 2 NpNs cos ϕs + γ 2 L 2 NsNi cos ϕs cos ϕi<br />

+ T 2 0 − w 2 pNsNi sin ϕs sin ϕi − γ 2 L 2 NsNi cos ϕs sin ϕi tan ρ0 sin α<br />

− γ 2 L 2 NpNs sin ϕs tan ρ0 sin α + γ 2 L 2 NsNi cos ϕi sin ϕs tan ρ0 sin α<br />

− γ 2 L 2 NsNi sin ϕs sin ϕi tan ρ0 2 sin α 2 + γ 2 L 2 NpNi sin ϕi tan ρ0 sin α.<br />

(A.5)<br />

This set of expressions is far more useful than compact. The matrix terms<br />

become simpler in some particular spdc configurations that are treated in<br />

chapters 2 and 4. For instance, when the pump polarization is parallel to the<br />

x axis, the matrix terms become<br />

a =w 2 p + 2w 2 s + γ 2 L 2 tan ρ 2 0<br />

b =w 2 p cos ϕs 2 + 2w 2 s + γ 2 L 2 sin ϕs 2<br />

c =w 2 p + 2w 2 i + γ 2 L 2 tan ρ 2 0<br />

d =w 2 p cos ϕi 2 + 2w 2 i + γ 2 L 2 sin ϕi 2<br />

f = 2<br />

B2 s<br />

g = 2<br />

B2 i<br />

+ T 2 0 + γ 2 L 2 (Np − Ns cos ϕs) 2 + w 2 pN 2 s sin ϕs 2<br />

+ T 2 0 + γ 2 L 2 (Np − Ni cos ϕi) 2 + w 2 pN 2 i sin ϕi 2<br />

h =m = −γ 2 L 2 sin ϕs tan ρ0<br />

i =w 2 p + γ 2 L 2 tan ρ0 2<br />

j =s = γ 2 L 2 sin ϕi tan ρ0<br />

k =t = γ 2 L 2 tan ρ0(Np − Ns cos ϕs)<br />

l =u = γ 2 L 2 tan ρ0(Np − Ni cos ϕi)<br />

n = − γ 2 L 2 sin ϕs sin ϕi + w 2 p cos ϕs cos ϕi<br />

p = − γ 2 L 2 sin ϕs(Np − Ns cos ϕs) − w 2 pNs cos ϕs sin ϕs<br />

r = − γ 2 L 2 sin ϕs(Np − Ni cos ϕi) + w 2 pNi cos ϕs sin ϕi<br />

v =γ 2 L 2 sin ϕi(Np − Ns cos ϕs) − w 2 pNs cos ϕi sin ϕs<br />

w =γ 2 L 2 sin ϕi(Np − Ni cos ϕi) + w 2 pNi cos ϕi sin ϕi<br />

z =γ 2 L 2 N 2 p − γ 2 L 2 Np(Ni cos ϕi + Ns cos ϕs) + γ 2 L 2 NsNi cos ϕs cos ϕi<br />

+ T 2 0 − w 2 pNsNi sin ϕs sin ϕi.<br />

(A.6)<br />

The matrix notation extends to functions of the mode function. For instance,<br />

the purity of the spatial part of the two-photon state, given by equation 2.11,<br />

65

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