Difference between revisions of "Neutron Polarimeter"
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Line 11: | Line 11: | ||
<math> E = p^2 + m^2</math> | <math> E = p^2 + m^2</math> | ||
− | writing four-vectors: | + | writing four-vectors:<br> |
− | |||
<math> p_{\gamma} = \left( T_{\gamma},\ T_{\gamma},\ 0,\ 0 \right) </math> | <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_D = \left( m_D,\ 0,\ 0,\ 0 \right) </math> | ||
Line 19: | Line 18: | ||
− | Doing four-vector algebra: | + | Doing four-vector algebra:<br> |
− | |||
<math> p^{\mu}_{\gamma} + p^{\mu}_D = p^{\mu}_p + p^{\mu}_n \Rightarrow </math><br> | <math> p^{\mu}_{\gamma} + p^{\mu}_D = p^{\mu}_p + p^{\mu}_n \Rightarrow </math><br> | ||
<math> p^{\mu\ 2}_p = \left(p^{\mu}_{\gamma} + p^{\mu}_D - p^{\mu}_n\right)^2 = | <math> p^{\mu\ 2}_p = \left(p^{\mu}_{\gamma} + p^{\mu}_D - p^{\mu}_n\right)^2 = |
Revision as of 03:26, 7 June 2010
Analysis of energy dependence
four-vectors algebra
writing four-vectors:
Doing four-vector algebra:
Detector is located at
, so
and visa versa
plots
low energy approximation
As we can see from Fig.2 for low energy neutrons (0-21 MeV)
energy dependence of incident photons is linear
Find that dependence. We have:
So, the equation of the line is:
Finally for low energy neutrons (0-21 MeV):