The “color” of light is generally identified by the distribution of power or intensity as a function of wavelength λ. Visible light has a wavelength that ranges from about 400 nm to just over 700 nm. Sometimes it is convenient to describe light in terms of units called “wavenumbers,” where the wavenumber w is typically measured in units of cm^{-1} (“inverse centimeters”) and is simply equal to the inverse of the wavelength, and is therefore proportional to frequency:

In applications like Raman spectroscopy, both wavelength and wavenumber units are often used together, leading to potential confusion. The laser lines are generally identified by wavelength, but the separation of a particular Raman line from the laser line is generally given by a “wavenumber shift” Δw, since the frequency of the response is fixed by the molecular properties of the material and independent of which laser wavelength is used to excite the line.

When speaking of a “shift” from a first known wavelength λ_{1} to a second known wavelength λ_{2}, the resulting wavelength shift Δλ is given by

whereas the resulting wavenumber shift Δw is given by

When speaking of a known wavenumber shift Δw from a first known wavelength λ_{1}, the resulting second wavelength λ_{2} is given by

Note that when the final wavelength λ_{2} is longer than the initial wavelength λ_{1}, which corresponds to a “red shift,” in the above equations Δw < 0, consistent with a shift toward smaller values of w. However, when the final wavelength λ_{2} is shorter than the initial wavelength λ_{1}, which corresponds to a “blue shift,” Δw > 0, consistent with a shift toward larger values of w.