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Doppler-shift Correction of Emitted tex2html_wrap_inline82 -Rays

  figure15
Figure 1: Experimental set-up with double ionization chamber and Ge-detector positioned at tex2html_wrap_inline86 .

A.) special geometry: Ge-detector at tex2html_wrap_inline84

Doppler-shift correction:

displaymath21

where tex2html_wrap_inline88 is the measured Doppler-shifted tex2html_wrap_inline82 -ray energy

tex2html_wrap_inline92 for an excited fragment in det-1
tex2html_wrap_inline94 for an excited fragment in det-2

tex2html_wrap_inline96 is the polar emission angle of excited fragment and tex2html_wrap_inline98 the fragment velocity

displaymath30

B.) general case: Ge-detector at tex2html_wrap_inline102

Doppler-shift correction:

displaymath21

where tex2html_wrap_inline88 is the measured Doppler-shifted tex2html_wrap_inline82 -ray energy

eqnarray45

eqnarray54

for an excited fragment in det-1 and in det-2, respectively.

tex2html_wrap_inline96 is the polar emission angle of excited fragment and tex2html_wrap_inline98 the fragment velocity

displaymath30

  figure67
Figure 2: Fragment mass selected tex2html_wrap_inline82 -ray spectra: no Doppler-shift correction (top), Doppler-shift correction for the light fragment mass (center) and Doppler-shift correction for the heavy fragment mass (bottom).




last update: 16.08.2002 Hans-Juergen Wollersheim HJW