Difference between revisions of "Neutron Polarimeter"
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energy dependence of incident photons is linear | energy dependence of incident photons is linear | ||
− | Find that dependence. We have: | + | Find that dependence. We have:<br> |
− | |||
<math> T_{\gamma}(0\ MeV) = 1.715360792\ MeV </math> | <math> T_{\gamma}(0\ MeV) = 1.715360792\ MeV </math> | ||
<math> T_{\gamma}(21\ MeV) = 44.78703086\ MeV </math> | <math> T_{\gamma}(21\ MeV) = 44.78703086\ MeV </math> | ||
− | So, the equation of the line is: | + | So, the equation of the line is:<br> |
− | |||
<math> T_{\gamma}(T_n) | <math> T_{\gamma}(T_n) | ||
= \frac{T_{\gamma}(21\ MeV) - T_{\gamma}(0\ MeV)}{21\ MeV - 0\ MeV}\ T_n + T_{\gamma}(0\ MeV) </math> | = \frac{T_{\gamma}(21\ MeV) - T_{\gamma}(0\ MeV)}{21\ MeV - 0\ MeV}\ T_n + T_{\gamma}(0\ MeV) </math> |
Revision as of 03:17, 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):