Difference between revisions of "Doppler Broadening"
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− | =Theory of | + | Spent fuel casket density: |
− | == Photon emmision along direction of fission fragment | + | |
+ | =Theory of Doppler Broadening= | ||
+ | == Photon emmision along direction of fission fragment velocity== | ||
<math>E_{shift} = E_{photon} \frac{1-\beta \cos(\theta_{photon}^i)}{\sqrt{1-\beta_i^2}}</math> = amount of energy the gamma ray was shifted by | <math>E_{shift} = E_{photon} \frac{1-\beta \cos(\theta_{photon}^i)}{\sqrt{1-\beta_i^2}}</math> = amount of energy the gamma ray was shifted by | ||
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= Cf-252 Fission = | = Cf-252 Fission = | ||
The table below from http://www-aix.gsi.de/~wolle/ identifies gamma energies (in keV) for several fission fragments of Cf-252. | The table below from http://www-aix.gsi.de/~wolle/ identifies gamma energies (in keV) for several fission fragments of Cf-252. | ||
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+ | [[Image:Cf-252_FF_Egamma_Table.gif]][[Image:Cf-252_FF_Egamma_Table1.jpg]] | ||
+ | [[Image:Cf-252_FF_Egamma_Table2.jpg]][[Image:Cf-252_FF_Egamma_Table3.jpg]] | ||
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==Photon Spectra from Cf-252 == | ==Photon Spectra from Cf-252 == | ||
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[[July 3,2007 Cf-252 without lead container measurements with HpGe & fast plastic scintillators in coincidence]]<br> | [[July 3,2007 Cf-252 without lead container measurements with HpGe & fast plastic scintillators in coincidence]]<br> | ||
[[July 6, 2007 Neutron Capture in lead]]<br> | [[July 6, 2007 Neutron Capture in lead]]<br> | ||
+ | [[July 10, 2007 Division of gated to ungated spectra of Cf-252]]<br> | ||
+ | [[July 11, 2007 Experimental setup]]<br> | ||
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[[Results and Discussion]]<br> | [[Results and Discussion]]<br> | ||
Latest revision as of 07:48, 7 December 2008
Spent fuel casket density:
Theory of Doppler Broadening
Photon emmision along direction of fission fragment velocity
= 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
The table below from http://www-aix.gsi.de/~wolle/ identifies gamma energies (in keV) for several fission fragments of Cf-252.
Photon Spectra from Cf-252
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
June 19, gamma-singles spectra of a Cf-252 source
June 25,2007 Cf-252 measurements of gamma-spectrum using HpGe ungated
June 25,2007 Cf-252 measurements of total gamma-spectrum using HpGe ungated
June 27,2007 Cf-252 measurements with HpGe detector and BC408
July 3,2007 Cf-252 without lead container measurements with HpGe & fast plastic scintillators in coincidence
July 6, 2007 Neutron Capture in lead
July 10, 2007 Division of gated to ungated spectra of Cf-252
July 11, 2007 Experimental setup
Measurements at the IAC
File:HuntsIACgraphs.pdf
File:Promptg02 cf252 IAC.pdf
Details of Cf-252 Source
The manufacturers description of the source File:CF-252-Description.pdf
Gamma and Neutron activity curvesFile:CF-252-gamma-n-activitycurves.pdf