The Stokes shift in Raman spectroscopy corresponds to a decrease in energy due to the interaction with the sample. The Stokes line is observed at a frequency \( \nu_{\text{Stokes}} \) given by:
\[
\nu_{\text{Stokes}} = \nu_{\text{vibration}} - \frac{c}{\lambda}.
\]
where \( \lambda = 532 \, \text{nm} \) is the laser wavelength. Converting the wavelength to cm:
\[
\lambda = 532 \times 10^{-7} \, \text{cm}.
\]
The shift in frequency is:
\[
\frac{c}{\lambda} = \frac{3.0 \times 10^8}{532 \times 10^{-9}} = 5.64 \times 10^{13} \, \text{Hz}.
\]
The corresponding frequency shift is \( 5.64 \times 10^{13} \, \text{Hz} \), which corresponds to the Stokes line. Thus, the frequency observed is:
\[
\nu_{\text{Stokes}} = 560 - 5.64 \times 10^{-2} \, \text{cm}^{-1} \approx 554 \, \text{cm}^{-1}.
\]
Thus, the Stokes line will be observed at \( 554 \, \text{cm}^{-1} \).