Difference between revisions of "Doppler Broadening"
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FWHM(for energy 2617 keV)=2.5 keV(experimental data)<br> | FWHM(for energy 2617 keV)=2.5 keV(experimental data)<br> | ||
− | Energy difference <math>E_{shift180^0}</math>-<math>E_{shift90^0}</math>=172.8 keV | + | Energy difference <math>E_{shift180^0}</math>-<math>E_{shift90^0}</math>=172.8 keV. This result shows us that we do not have Doppler Shift.<br> |
== Photon emission off fission fragment velocity axis== | == Photon emission off fission fragment velocity axis== |
Revision as of 19:49, 25 June 2007
Theory of Dopler Broadening
Photon emmision along direction of fission fragment velocit
= amount of energy the gamma ray was shifted by
where
=- for an excited fragment in det-2
is the polar emission angle of excited fragment and the fragment velocity
Our Calculations
For example for energy E=2617 keV and the fragment velocity v=
We obtained the following results for different angles between the direction of the fission fragment propagation and the direction of the gamma emission
(i)
(ii)
(iii)
FWHM(for energy 2617 keV)=2.5 keV(experimental data)
Energy difference
Photon emission off fission fragment velocity axis
Cf-252 Fission
Photon Spectra from Cf-252
References: http://prola.aps.org/pdf/PR/v104/i3/p699_1
Smith, A. B.; Fields, P. R.; Friedman A. M., Physical Review, vol. 104, Issue 3, pp. 699 - 702
Measurements in the Beam test lab with HpGe and BC408
June 15,2007 Cf-252 measurements with HpGe & neutron sensitive scintillators in coincidence
June 19,2007 Cf-252 measurements with HpGe & neutron sensitive scintillators in coincidence
June 19,2007 Cf-252 measurements of gamma-spectrum using HpGe ungated