BROADR:
Typical Broadened Cross Sections





The effects of temperature on typical cross sections is best illustrated by giving several examples. First, here is the (n,α) cross section for B-10 shown for temperatures of 0K, 3000K, and 3000000K. This shows that a 1/v cross section is invariant under Doppler broadening.

Postscript Figure

Next, here is the elastic cross section for carbon shown for temperatures of 0K, 300K, 3000K, and 30000K. This shows that a constant cross section will develop a 1/v tail under Doppler broadening.

Postscript Figure

Finally, here is how resonance cross section behave under Doppler broadening. The (n,gamma) cross section for Pu-240 is shown for temperatures of 0K, 30000K, and 300000K. Resonances with energies larger than kT/A broaden symmetrically (and their areas tend to remain constant). Low energy resonances develop an additional 1/v tail, and their areas do not remain constant under Doppler broadening.

Postscript Figure

These effects are best understood by noting that Doppler broadening preserves the reaction rate v*σ(v), and a finite reaction rate is expected for T larger than zero even as v goes to zero.


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23 January 2013 T-2 Nuclear Information Service ryxm@lanl.gov