A nucleus of mass \( M \) emits \( \gamma \)-ray photon of frequency ‘\( v \)’. The loss of internal energy by the nucleus is: [Take ‘\( c \)’ as the speed of electromagnetic wave]
\( h \,v \)
\( h \,v \left[ 1 + \dfrac{hv}{2 M c^2} \right] \)
\( 0 \)
\( h v \left[ 1 - \dfrac{h v}{2 M c^2} \right] \)