The heat capacity of a monatomic ideal gas is governed by how many independent ways its molecules can store kinetic energy. Let's work through each option using this idea.
A monatomic gas molecule has only 3 translational degrees of freedom (no rotational or vibrational modes contribute at ordinary temperatures), so by the equipartition theorem its molar internal energy is \[ U = \frac{3}{2}RT \] which gives a molar heat capacity of \[ C = \frac{3}{2}R = 1.5R \]
Since a monatomic gas stores energy only through translational motion, its heat capacity works out to \( \tfrac{3}{2}R \).
Therefore, the correct answer is 1.5R.