Step 1: Use of the photoelectric equation.
The photoelectric equation is given by:
\[
\frac{hc}{\lambda} = \phi + eV_s
\]
where \( h \) is Planck's constant, \( c \) is the speed of light, \( \lambda \) is the wavelength, \( \phi \) is the work function, and \( V_s \) is the stopping potential.
Step 2: Solving for the wavelength.
Rearranging the equation to solve for \( \lambda \), we get:
\[
\lambda = \frac{hc}{\phi + eV_s}
\]
Step 3: Conclusion.
Thus, the wavelength of the incident radiation is \( \frac{hc}{\phi + eV_s} \), corresponding to option (B).