Step 1: In the quantum harmonic oscillator, the position and momentum operators \( \hat{X} \) and \( \hat{P} \) can be expressed in terms of the raising and lowering operators. The matrix elements of these operators in the energy eigenbasis are non-zero only for certain transitions.
Step 2: The matrix element \( \langle m | \hat{P} \hat{X} | n \rangle \) is non-zero when \( m = n \) or when \( m = n \pm 2 \). This condition arises from the properties of the creation and annihilation operators.
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: