I am using a laser source that is wider than typical laser source for Raman spectroscopy. This mean that the full width at half maximum (FWHM) of the laser is about 5-10 nm, compared to the normal 1-3 nm. 

Hypothetically, if my laser source peaks at 785 nm and has a FWHM of 10nm, this means:

  • Assuming that it is 10,000 units at the peak (785 nm)
  • Then I could expect 5,000 units per second at around 780 nm and 790 nm
  • The intensity of the wavelengths of 780 to 785 and 790 to 785 follows a non-linear function that I can probably characterize.

If I look at a particular wavenumber in my result:

Can I express it as the sum of overlapping Raman spectras from different wavelengths? 

This implies: intensity2000 = SUMMATION( ... a780 * intensity780 + a781 * intensity781 + ....), where a780 = 0.5 and a790 = 0.5, etc 

I am interested to know whether there are research done in this area that could enable me to use a wider, but much cheaper, laser source. 

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