solving part by part,\
Equation (1)\\
Need to show that the below Equation (2)
\small
$$\Omega_dm =0.3 h^{-2} (\frac{x_f}{10})(\frac{g_*(m)}{100})^\frac{1}{2} \frac{10^{-37}cm^2}{\langle\sigma\nu\rangle}$$
Equation(2 )\ follows from the first equation when baryons are neglected.
\small...
Hi add the values the equation but I'm still not getting the numerator part, because I'm missing the ##g_*##, and ##x_f##. For me to add that is it fine to include those to the equation ? or what's the best move?
ok, if I plug in the nominal values into the equation
$$\Omega_dm =\sqrt[]{\frac{4\pi^3G}{45}*g_*(m)}\frac{1}{\langle \sigma\nu\rangle}\frac{x_fT_0^3}{30\rho_cr}$$
$$\Omega_m =\sqrt[]{\frac{4\pi^3
10^{19} GeV }{45}*g_*(m)}\frac{1}{\langle...
Noted, but 0.3 comes as the magnitude of the when applying to the equation. As per the notes given I took magnitude of that to apply into the equation. This is when the freeze-out begins.
The fraction of critical density due to dark matter today,
$$\Omega_{X0}$$ , equation given as...
then Equation(1.1) becomes,\
$$\Omega_dm = 0.3 h^{-2} (\frac{g_*(m)}{100})^\frac{1}{2}\frac{1}{\langle \sigma\nu\rangle}(\frac{x_f}{10}) \sqrt[]{\frac{4\pi^3}{45}}10^{19}Gev[\frac{(10^{-13} GeV)^3}{30*1.054*10^{-5}\frac{GeV}{cm^3}}] $$
Equation( 1.2)Converting the GeV to eV and Joules got the...
Please refer to the below,
$$\Omega_x = \sqrt[]{\frac{4\pi^3G}{45}*g_*(m)}\frac{1}{\langle \sigma\nu\rangle}\frac{x_fT_0^3}{30\rho_cr}$$\\
Considering the facts at WIMP dark matter ,
$$\Omega_X \approx\Omega_dm\approx0.3$$
considering
$$\rho_cr = 1.054h^2 10^{-5} \frac{GeV}{cm^3}$$...