A slow-neutron capture resonance in an even-even nuclide of mass number (target spin…

PHYSICS · Multi-part · Fermi University Physics · Nuclear Physics · Nuclear reactions · Nuclear reactions

The Nucleus Resolved, Ch Reaction mechanisms: resonances, the compound nucleus, direct reactions and the optical model

Problem

A slow-neutron capture resonance in an even-even nuclide of mass number A=114A = 114 (target spin 00) is studied by measuring the radiative-capture cross section σγ\sigma_\gamma at several neutron energies: E (eV)E\,(\mathrm{eV}): 1.30, 1.40, 1.45, 1.50, 1.55, 1.60, 1.701.30,\ 1.40,\ 1.45,\ 1.50,\ 1.55,\ 1.60,\ 1.70 σγ (b)\sigma_\gamma\,(\mathrm{b}): 70.6, 240, 600, 1200, 600, 240, 70.670.6,\ 240,\ 600,\ 1200,\ 600,\ 240,\ 70.6 ((a)) From the table, read off the resonance energy ErE_r and the total width Γ\Gamma, using the points where the cross section has fallen to half its peak value. ((b)) Given that for this resonance Γn≪Γγ\Gamma_n \ll \Gamma_\gamma (as for the 6.67 eV6.67\,\mathrm{eV} level of 238U^{238}\mathrm{U}), so that Γ≈Γγ\Gamma \approx \Gamma_\gamma, state Γγ\Gamma_\gamma. ((c)) Using σγ,peak=4πλˉ2gstatΓnΓγΓ2\sigma_{\gamma,\rm peak} = 4\pi\bar\lambda^2 g_{\rm stat}\dfrac{\Gamma_n\Gamma_\gamma}{\Gamma^2} with gstat=1g_{\rm stat}=1 and the reduced neutron wavelength λˉ=ℏc/2mnc2Er\bar\lambda = \hbar c/\sqrt{2m_nc^2E_r} (non-relativistic), with mnc2=939.57 MeVm_nc^2 = 939.57\,\mathrm{MeV} and ℏc=197.327 MeV fm\hbar c = 197.327\,\mathrm{MeV\,fm}, find Γn\Gamma_n.

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