A hypothetical allowed emitter

PHYSICS · Multi-part · Fermi University Physics · Scientific Practice & Experimental Methods · Nuclear Physics · Radioactivity and decay modes

The Nucleus Resolved, Ch Beta decay: Fermi's theory, parity violation and the double beta modes

Problem

A hypothetical allowed β−\beta^- emitter, with the Coulomb factor of the daughter switched off (as in the model spectrum built for an allowed transition), gives the following counts NN in four equal-width momentum bins, at kinetic energies TeT_e: Te=0.1 MeVT_e = 0.1\,\mathrm{MeV}: N=718N = 718 Te=0.3 MeVT_e = 0.3\,\mathrm{MeV}: N=1428N = 1428 Te=0.5 MeVT_e = 0.5\,\mathrm{MeV}: N=1218N = 1218 Te=0.7 MeVT_e = 0.7\,\mathrm{MeV}: N=482N = 482 ((a)) For each bin, compute the electron momentum pecp_ec from TeT_e using W=1+Te/mec2W = 1 + T_e/m_ec^2 and pec=mec2W2−1p_ec = m_ec^2\sqrt{W^2-1}, with mec2=0.511 MeVm_ec^2 = 0.511\,\mathrm{MeV}. ((b)) Form the Kurie variable K=N/pecK = \sqrt{N}/p_ec at each bin and show the four points lie on a straight line in TeT_e. ((c)) Extrapolate the line to find the endpoint energy QQ.

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