(d) If the applied force is less than limiting friction between block $A$ and $B$ , then whole system move with common acceleration
$i.e.$ $a_{A} = a_{B} = \frac{F}{m_{A} + m_{B}}$
but the applied force increases with time, so when it becomes more than limiting friction between $A$ and $B$, block $B$ starts moving under the effect of net force $F - F_{k}$ Where $F_{k} =$ kinetic friction between block $A$ and $B$
$\therefore$ Acceleration of block $B$, $a_{B} = \frac{F - F_{k}}{m_{B}}$
As $F$ is increasing with time so $a_{B}$ will increase with time
Kinetic friction is the cause of motion of block $A$
$\therefore$ Acceleration of block $A$, $a_{A} = \frac{F_{k}}{m_{A}}$
It is clear that $a_{B} > a_{A}$. $i.e.$ graph (d) correctly represents the variation in acceleration with time for block $A$ and $B$