JEE Challenger
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Kinetic Energy Range of Electron with Massive Anti Neutrino

Comprehension Passage

The process of β\beta-decay, discovered around 1900, fundamentally involves the decay of a neutron (nn). In laboratory observations, a proton (pp) and an electron (e−e^-) appear as the products of neutron decay. Hence, treating the neutron decay as a two-body process led to theoretical predictions that the kinetic energy of the emitted electron would remain constant. However, experimental findings revealed a continuous energy spectrum for the electron. To resolve this, Pauli proposed a three-body decay model in 1930, represented by n→p+e−+νˉen \rightarrow p + e^- + \bar{\nu}_e. Under the assumption that the anti-neutrino (νˉe\bar{\nu}_e) is massless with minimal energy, and taking the initial neutron to be stationary, principles of conservation of momentum and energy were employed. Calculations yielded a maximum electron kinetic energy of 0.8×106 eV0.8 \times 10^6\text{ eV}, with the proton carrying negligible recoil kinetic energy.

Assuming the anti-neutrino possesses a rest mass of 3 eV/c23\text{ eV}/c^2 (where cc represents the speed of light) instead of being massless, what would be the valid range for the electron's kinetic energy KK?

Options

A

0≤K≤0.8×106 eV0 \le K \le 0.8 \times 10^6\text{ eV}

B

3.0 eV≤K≤0.8×106 eV3.0\text{ eV} \le K \le 0.8 \times 10^6\text{ eV}

C

3.0 eV≤K<0.8×106 eV3.0\text{ eV} \le K < 0.8 \times 10^6\text{ eV}

D

0≤K<0.8×106 eV0 \le K < 0.8 \times 10^6\text{ eV}

Correct

Step-by-Step Solution

To determine the valid range of the electron's kinetic energy KK when the anti-neutrino has a non-zero rest mass, we analyze the decay process:

n→p+e−+νˉen \rightarrow p + e^- + \bar{\nu}_e

  1. Lower Bound of Kinetic Energy (KminK_{\text{min}}): The electron can be produced nearly at rest, with its momentum balanced by the proton and the anti-neutrino. Therefore, the minimum possible kinetic energy for the electron remains: Kmin=0K_{\text{min}} = 0

  2. Upper Bound of Kinetic Energy (KmaxK_{\text{max}}): When the anti-neutrino is assumed to be massless (mνˉ=0m_{\bar{\nu}} = 0), its minimum total energy can approach zero (Eνˉ,min→0E_{\bar{\nu},\text{min}} \to 0), allowing the electron to achieve a maximum kinetic energy of: Kmax, massless=0.8×106 eVK_{\text{max, massless}} = 0.8 \times 10^6 \text{ eV}

    However, if the anti-neutrino has a finite rest mass mνˉ=3 eV/c2m_{\bar{\nu}} = 3\text{ eV}/c^2, its total energy EνˉE_{\bar{\nu}} must always be greater than or equal to its rest mass energy: Eνˉ=pνˉ2c2+(mνˉc2)2≥mνˉc2=3 eVE_{\bar{\nu}} = \sqrt{p_{\bar{\nu}}^2 c^2 + (m_{\bar{\nu}} c^2)^2} \ge m_{\bar{\nu}} c^2 = 3\text{ eV}

    Since the anti-neutrino carries away at least 3 eV3\text{ eV} of energy from the available decay energy QQ, the maximum kinetic energy that the electron can acquire is reduced by 3 eV3\text{ eV}: Kmax=0.8×106 eV−3 eV<0.8×106 eVK_{\text{max}} = 0.8 \times 10^6\text{ eV} - 3\text{ eV} < 0.8 \times 10^6\text{ eV}

  3. Conclusion: Combining the lower and upper bounds, the valid range for the electron's kinetic energy KK is: 0≤K<0.8×106 eV0 \le K < 0.8 \times 10^6 \text{ eV}

This corresponds to Option (D).