Continuous distribution of the electron energy:
In beta decay, the energy of the emitted electron is not fixed, but follows a continuous distribution. This is because the decay involves three particles: the neutron, proton, electron, and antineutrino. The energy of the electron is shared between these three particles, resulting in a continuous energy spectrum. This feature indicates that beta decay is a three-body decay process.
Therefore, (A) is correct.
Spin of the final state:
The spin of the final state is crucial for the decay process. In beta decay, the final state consists of a proton, an electron, and an antineutrino, and their spins are arranged in such a way that the angular momentum is conserved. This is possible only if there are three particles involved in the decay, confirming that it is a three-body decay.
Therefore, (B) is correct.
Mass of the electron:
The mass of the electron does not directly determine whether the decay is a three-body decay. While the electron mass affects the energy distribution in the decay, it is the presence of three particles in the final state that creates the continuous energy spectrum.
Therefore, (C) is incorrect.
Mass of the proton:
The mass of the proton does not directly imply that the decay must be a three-body decay. The number of particles involved in the decay process is what matters in determining whether it is a three-body decay.
Therefore, (D) is incorrect.
Consider two hypothetical nuclei \( X_1 \) and \( X_2 \) undergoing \( \beta \) decay, resulting in nuclei \( Y_1 \) and \( Y_2 \), respectively. The decay scheme and the corresponding \( J^P \) values of the nuclei are given in the figure. Which of the following option(s) is/are correct? (\( J \) is the total angular momentum and \( P \) is parity)
The figure shows an opamp circuit with a 5.1 V Zener diode in the feedback loop. The opamp runs from \( \pm 15 \, {V} \) supplies. If a \( +1 \, {V} \) signal is applied at the input, the output voltage (rounded off to one decimal place) is:
A wheel of mass \( 4M \) and radius \( R \) is made of a thin uniform distribution of mass \( 3M \) at the rim and a point mass \( M \) at the center. The spokes of the wheel are massless. The center of mass of the wheel is connected to a horizontal massless rod of length \( 2R \), with one end fixed at \( O \), as shown in the figure. The wheel rolls without slipping on horizontal ground with angular speed \( \Omega \). If \( \vec{L} \) is the total angular momentum of the wheel about \( O \), then the magnitude \( \left| \frac{d\vec{L}}{dt} \right| = N(MR^2 \Omega^2) \). The value of \( N \) (in integer) is: