(c) In hydrogen atom $E_{n} = - \frac{Rhc}{n^{2}}$
Also $E_{n} \propto m$; where $m$ is the mass of the electron. Here the electron has been replaced by a particle whose mass is double of an electron. Therefore, for this hypothetical atom energy in $n^{th}$ orbit will be given by $E_{n} = - \frac{2Rhc}{n^{2}}$
The longest wavelength $\lambda_{\max}$ (or minimum energy) photon will correspond to the transition of particle from $n = 3$ to $n = 2 \Rightarrow \frac{hc}{\lambda_{\max}} = E_{3} - E_{2} = 2Rhc\left( \frac{1}{2^{2}} - \frac{1}{3^{2}} \right)$
This gives $\lambda_{\max} = \frac{18}{5R}$