Laser based apparatus, methods and applications
Embodied is a two-color, fiber-delivered picosecond source for coherent Raman scattering (CRS) imaging. A wavelength tunable picosecond pump is generated by nonlinear spectral compression of a prechirped femtosecond pulse from a mode-locked titanium:sapphire (Ti:S) laser. A 1064-nm picosecond Stokes pulse is generated by an all-fiber time-lens source (or suitable alternative source) that is synchronized to the Ti:S laser. The pump and Stokes beams are combined in an optical fiber coupler, which serves not only as the delivery fiber but also as the nonlinear medium for spectral compression of the femtosecond pulse. CRS imaging of mouse skin is performed to demonstrate the practicality of this source.
1. An optical apparatus comprising:
a wavelength-tunable laser source that provides a pump beam output having a femtosecond pulse duration at a first desired wavelength through an output port of the pump beam laser source;
a prechirping apparatus optically coupled to the output port to provide a prechirped the femtosecond pump beam output at the first desired wavelength;
a light source assembly comprising at least one of a different laser source and a time-lense source having a Stokes pulse output having a picosecond pulse duration at a second desired wavelength that is different than the first desired wavelength; and
a fiber optic coupler having an input port optically coupled to both the prechirped femtosecond pump beam output at the first desired wavelength and the picosecond Stokes pulse output at the second desired wavelength, and having an optical output characterized by a spatially-overlapping, non-linearly-spectrally compressed pump beam output having a picosecond pulse duration and the Stokes picosecond pulse output.
2. The optical apparatus of claim 1 wherein the pump beam laser source comprises a Ti:S mode-locked laser source.
3. The optical apparatus of claim 1 wherein the different laser source comprises a continuous wave laser source.
4. The optical apparatus of claim 1 wherein the time-lens source comprises an all-fiber time-lens source.
5. The optical apparatus of claim 1 wherein the coupler comprises a 2×2 fiber coupler.
6. The optical apparatus of claim 1 further comprising a microscope optically coupled to the spatially-overlapping, wavelength-tunable, non-linearly-spectrally compressed pump beam output having a picosecond pulse duration and the Stokes picosecond pulse output.
7. The optical apparatus of claim 1 wherein:
the first desired wavelength is 817 nanometers (nm); and
the second desired wavelength is 1064 nm.
8. The apparatus of claim 1 , wherein the fiber optic coupler is a 2×2 coupler.
9. The apparatus of claim 1 , wherein the fiber optic coupler is a wavelength division multiplexer (WDM).
10. The apparatus of claim 1 , wherein the prechirped the first laser femtosecond pump beam output is negatively prechirped.
11. An imaging method comprising:
generating a prechirped laser pump beam having a femtosecond pulse duration at first desired wavelength;
generating a Stokes pulse output having a picosecond pulse duration at a second desired wavelength that is different than the first desired wavelength;
inputting the prechirped femtosecond laser pump beam to a fiber optic coupler to obtain an nonlinearly spectrally compressed, picosecond duration laser pump beam in the fiber optic coupler;
inputting the Stokes picosecond pulse output in the fiber optic coupler to spatially overlap the picosecond duration, nonlinearly spectrally compressed laser pump beam and the Stokes picosecond pulse output;
inputting the spatially-overlapped, non-linearly-spectrally compressed, picosecond duration pump beam output and the Stokes picosecond pulse output from the fiber optic coupler to a microscope; and
illuminating a sample to be imaged with the spatially-overlapped, non-linearly-spectrally compressed, picosecond duration pump beam output and the Stokes picosecond pulse output.
12. The method of claim 11 wherein the sample comprises a biological specimen.
13. The method of claim 11 , further comprising collecting a Raman signal from the sample.
14. The method of claim 11 , further comprising providing a 2×2 fiber coupler for nonlinearly spectrally compressing the negatively prechirped laser pump beam.
15. The method of claim 11 , further comprising providing a fiber wavelength division multiplexer (WDM) for nonlinearly spectrally compressing the prechirped laser pump beam.
16. The method of claim 11 , further comprising generating a negatively prechirped laser pump beam having a femtosecond pulse duration at a first desired wavelength.
17. The method of claim 11 , further comprising temporally overlapping the non-linearly-spectrally compressed, picosecond duration pump beam output and the Stokes picosecond pulse output.