A method for obtaining a polarized orbital angular momentum Raman spectrum using vector vortex beams, includes the steps of emitting a polarized laser light from a laser source. The polarized laser light is passed through a narrow band filter that is then passed through a section of wave plates (quarter or half wave plate) to generate polarized light (linear, circular, radial and azimuthal), then through a q-plate (vortex retarder or spiral plate) to give a vortex structure topology carrying orbital angular momentum with a helical phase. The polarized vector vortex light is then directed to contact a sample, thereby producing a Raman scatter beam. The Raman scatter beam is passed back and collected into a spectrometer, thereby obtaining a Raman scattering spectrum of the sample to investigate the matching of the multipoles of the material and the multipoles of the light. A method for transmission with Multiple expansions of orbital angular momentum in rat cerebellum tissue is also disclosed. In general, we use polarized Laguerre-Gaussian vector vortex beams as a topology multipole model to describe and study the light matter interaction for Raman and transmission using the fact that the optical vortices and material can possess Multipoles denoted as L in form of monopole (L=0), dipole (L=1), quadrupole (L=2), octupole (L=3), hexidecapole (L=4) and higher orders. These multipoles can be involved with the matching up with the symmetry of the moments involved with vibrational states in Raman processes.
4 which follow the envelope of optical field of the laser gives rise to extreme broadening without HHG. The resulting spectra extend on the Stokes side towards the IR, RF to DC covering most of the electromagnetic spectrum. These HHG and Super broadening covering UUV to X rays and possibly to gamma ray regime for microscopes.
H01S 3/10 - Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating
H01S 3/00 - Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
H01S 3/108 - Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating by controlling devices placed within the cavity using non-linear optical devices, e.g. exhibiting Brillouin or Raman scattering
H01S 3/107 - Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating by controlling devices placed within the cavity using electro-optic devices, e.g. exhibiting Pockels or Kerr effect
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