JEE Advanced 2012 Paper 2 Physics Q12

Physics · Nuclei & Radioactivity

Problem

Paragraph for Questions 11 and 12 The β\beta-decay process, discovered around 1900, is basically the decay of a neutron (n)(n). In the laboratory, a proton (p)(p) and an electron (e−)(e^-) are observed as the decay products of the neutron. Therefore, considering the decay of a neutron as a two-body decay process, it was predicted theoretically that the kinetic energy of the electron should be a constant. But experimentally, it was observed that the electron kinetic energy has a continuous spectrum. Considering a three-body decay process, i.e. n→p+e−+νˉen\to p+e^-+\bar\nu_e, around 1930, Pauli explained the observed electron energy spectrum. Assuming the anti-neutrino (νˉe)(\bar\nu_e) to be massless and possessing negligible energy, and the neutron to be at rest, momentum and energy conservation principles are applied. From this calculation, the maximum kinetic energy of the electron is 0.8×106 eV0.8\times10^6\,\mathrm{eV}. The kinetic energy carried by the proton is only the recoil energy. If the anti-neutrino had a mass of 3 eV/c23\,\mathrm{eV}/c^2 (where cc is the speed of light) instead of zero mass, what should be the range of the kinetic energy, KK, of the electron?

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