Step 1: Convert the Rydberg constant into an energy scale instead of a wavenumber.
The quantity $hcR$ is the well known ground-state binding energy of hydrogen, $hcR \approx 13.6\text{ eV}$, so transition energies can be written directly in eV as $\Delta E = 13.6\left(\dfrac{1}{n_1^2}-\dfrac{1}{n_2^2}\right)$.
Step 2: Identify the transition.
The Pfund series ends at $n_1 = 5$, and its first line comes from the very next level, $n_2 = 6$.
Step 3: Compute the transition energy. \[ \Delta E = 13.6\left(\frac{1}{25}-\frac{1}{36}\right) = 13.6\times\frac{11}{900} \approx 0.166\text{ eV} \]
Step 4: Convert this energy to wavelength using $hc/e = 1240$ eV-nm. \[ \lambda = \frac{1240}{0.166} \] \[ \boxed{\lambda \approx 7458\text{ nm}} \]