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Definition of cross sections 1 - Moodle

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Resonances 33. The peak energy <strong>of</strong> a resonance may be negative, in the case where a level <strong>of</strong> thecompound nucleus is close to the state corresponding to the capture <strong>of</strong> a neutron bythe target but is located below this state (called a negative resonance).4. Intermediate and heavy isotopes are characterized by a high number <strong>of</strong> resonances. Itbecome possible to apply statistical studies on the resonance widths γ and <strong>of</strong> theirspacing D, corresponding to a given spin and parity. This statistical treatment is usefulfor the representation <strong>of</strong> the unresolved resonances in domain 10keV ≤ E ≤ 300keV.5. The neutron width is a function <strong>of</strong> the incident neutron energy and is written γ n (e exc ).The statistical treatment on the neutron width is applied on the random variable(18)x = γl n〈γ l n〉where the reduced neutron width γn l , a function <strong>of</strong> the angular momentum quantumnumber l, is defined asγn l = γ n (e exc )(19)v l (e exc ) √ e excwhere v l (e exc ) is a coefficient related to the penetrability <strong>of</strong> the potential barrier in thetarget nucleus.ENE6101: Week 4 Cross <strong>sections</strong> – 18/37

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