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Remy Moll
2025-09-18 17:46:52 +02:00
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@@ -73,7 +73,7 @@ where $alpha_B$ is the recombination coefficient, $C$ is the clumping factor, $a
Ionizing photons, i.e. photons with energies above $13.6 "eV"$, experience a large optical depth, which justifies the sharp cutoff of the ionization profile at the bubble radius $R_b = root(3, 3/ (4pi) V(M,z))$. The radial dependence of the ionized fraction is expressed through the Heaviside step function $theta_"H"$ and reads Ionizing photons, i.e. photons with energies above $13.6 "eV"$, experience a large optical depth, which justifies the sharp cutoff of the ionization profile at the bubble radius $R_b = root(3, 3/ (4pi) V(M,z))$. The radial dependence of the ionized fraction is expressed through the Heaviside step function $theta_"H"$ and reads
$ $
x_("HII")(r bar M, z) = theta_"H" lr([R_b (M, z) - r], size: #150%) x_("HII")(r bar M, z) = theta_"H" lr([R_b (M, z) - r], size: #150%)
$ $
=== Expression of the reionization signal === Expression of the reionization signal