Neutron Polarimeter
Revision as of 21:26, 5 June 2010 by Oborn (talk | contribs) (→energy dependence of outcoming neutron versus energy of incoming photons)
[math] E = T + m[/math] [math] E = p^2 + m^2[/math]
writing four-vectors:
[math] p_{\gamma} = \left( T_{\gamma},\ T_{\gamma},\ 0,\ 0 \right) [/math] [math] p_D = \left( m_D,\ 0,\ 0,\ 0 \right) [/math] [math] p_{n} = \left( E_n,\ p_n\cos(\Theta_n),\ p_n\sin(\Theta_n),\ 0 \right) [/math] [math] p_{p} = \left( E_p,\ p_p\cos(\Theta_p),\ p_p\sin(\Theta_p),\ 0 \right) [/math]
Doing four-vector algebra:
[math] p^{\mu}_{\gamma} + p^{\mu}_D = p^{\mu}_p + p^{\mu}_n \Rightarrow [/math]
[math] (p^{\mu}_p)^2 = (p^{\mu}_{\gamma} + p^{\mu}_D - p^{\mu}_n)^2 =
(p^{\mu}_{\gamma})^2 + (p^{\mu}_D)^2 + (p^{\mu}_n)^2 + 2p^{\mu}_{\gamma}p^{\mu}_D - 2p^{\mu}_n(p^{\mu}_{\gamma} + p^{\mu}_D)
\Rightarrow
m_p^2 = m_y^2(=0) + m_D^2 + m_n^2
[/math]