The given primitive vectors represent a body-centered cubic (BCC) lattice. To verify this, let's examine the structure.
The primitive vectors are given as:
\[ \vec{a}_1 = a\hat{i}, \quad \vec{a}_2 = a\hat{j}, \quad \vec{a}_3 = \frac{a}{2}(\hat{i} + \hat{j} + \hat{k}). \]
The BCC lattice is characterized by one atom at the corner and one at the center of the unit cell. To calculate the volume of the primitive cell, we can use the scalar triple product:
\[ \textbf{Volume of the primitive cell} = \left| \vec{a}_1 \cdot (\vec{a}_2 \times \vec{a}_3) \right|. \]
First, calculate the cross product \( \vec{a}_2 \times \vec{a}_3 \):
\[ \vec{a}_2 \times \vec{a}_3 = a\hat{j} \times \frac{a}{2}(\hat{i} + \hat{j} + \hat{k}) = \frac{a^2}{2}(\hat{i} - \hat{k}). \]
Now, calculate the dot product with \( \vec{a}_1 = a\hat{i} \):
\[ \vec{a}_1 \cdot (\vec{a}_2 \times \vec{a}_3) = a\hat{i} \cdot \frac{a^2}{2}(\hat{i} - \hat{k}) = \frac{a^3}{2}. \]
Thus, the volume of the primitive cell is \( \frac{a^3}{2} \). Therefore, the correct answer is option (A).
Two projectile protons \( P_1 \) and \( P_2 \), both with spin up (along the \( +z \)-direction), are scattered from another fixed target proton \( T \) with spin up at rest in the \( xy \)-plane, as shown in the figure. They scatter one at a time. The nuclear interaction potential between both the projectiles and the target proton is \( \hat{\lambda} \vec{L} \cdot \vec{S} \), where \( \vec{L} \) is the orbital angular momentum of the system with respect to the target, \( \vec{S} \) is the spin angular momentum of the system, and \( \lambda \) is a negative constant in appropriate units. Which one of the following is correct?

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:
