Difference between revisions of "Neutron Polarimeter"
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=Relativistic kinematic= | =Relativistic kinematic= | ||
− | ==neutron | + | ==energy dependence of outcoming neutron versus energy of incoming photons== |
[[File:Collision.png|left|400px]] | [[File:Collision.png|left|400px]] | ||
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<math> p_{n} = \left( E_n,\ p_n\cos(\Theta_{n}),\ p_n\sin(\Theta_{n}),\ 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> | <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} </math> | <math> p^{\mu}_{\gamma} + p^{\mu}_{D} = p^{\mu}_{p} + p^{\mu}_{n} </math> | ||
− | <math> p^{\mu}_{ | + | <math> (p^{\mu}_{p})^2 = (p^{\mu}_{\gamma} + p^{\mu}_{D} - p^{\mu}_{n})^2 </math> |