Compact Raman generators

Patent metadata

Field	Value
Publication number	US-9438006-B2
Application number	US-201213476687-A
Country	US
Kind code	B2
Filing date	May 21, 2012
Priority date	May 21, 2012
Publication date	Sep 6, 2016
Grant date	Sep 6, 2016

Abstract

According to an embodiment of the disclosure, a Raman generator includes a Raman medium and one or more optical elements. The Raman medium is configured to receive a pump pulse at a first wavelength and shift at least a portion of the pump pulse energy or power into a Stokes-shifted pulse at a second wavelength. The one or more optical elements are configured to pass the pump pulse and the Stokes-shifted pulse multiple times through the Raman medium. Each pass of the pulses through the Raman medium follows a path. Each path is parallel or anti-parallel to the other paths.

First claim

What is claimed is:

1. A Raman generator comprising:
a Raman medium configured to receive a pump pulse at a first wavelength and shift at least a portion of the pump pulse energy or power into a Stokes-shifted pulse at a second wavelength, the Raman medium having a longitudinal central axis; and
one or more optical elements configured to pass the pump pulse and the Stokes-shifted pulse multiple times through the Raman medium;
wherein each pass of the pulses through the Raman medium follows a path;
wherein each path is parallel or anti-parallel to the other paths; and
wherein the paths of three or more consecutive passes of the pulses through the Raman medium alternate between opposite sides of the longitudinal central axis of the Raman medium.

2. The Raman generator of claim 1 , wherein
for each pass through the Raman medium, at least a portion of the pump pulse energy or power is shifted into the Stokes-shifted pulse at the second wavelength; and
the one or more optical elements are configured to pass both the pump pulse and the Stokes-shifted pulse along multiple common paths through the Raman medium, the multiple passes increasing a power of the Stokes-shifted pulse.

3. The Raman generator of claim 1 , further comprising:
at least two lenses configured to limit diffractive spreading of the pump pulse and the Stoke-shifted pulse.

4. The Raman generator of claim 1 , wherein the one or more optical elements comprise two prisms of different size.

5. The Raman generator of claim 1 , further comprising two lenses and two prism-lens combinations, wherein:
prism portions of the prism-lens combinations are configured to pass both the pump pulse and the Stokes-shifted pulse more than two times through the Raman medium, and
lens portions of the prism-lens combinations and the two lenses are configured to limit diffractive spreading of the pump and Stokes-shifted pulse.

6. The Raman generator of claim 1 , wherein the Raman generator provides an optical length of one meter in a package having a maximum dimension of thirty centimeters.

7. The Raman generator of claim 1 , wherein the received pulse is configured to pass through the Raman medium nine times.

8. The Raman generator of claim 1 , further comprising a spectral filter configured to control a spectral width of the Stokes-shifted pulse.

9. The Raman generator of claim 1 , wherein the Raman generator is configured such that the optical path and polarizations of the pump pulse and Stokes-shifted pulse are matched to preferred crystal axes in the Raman medium.

10. The Raman generator of claim 1 , wherein a conversion efficiency of the Raman generator determined by comparing the pump pulse initially received at the first wavelength to the generated Stokes-shifted pulse at the second wavelength is greater than or equal to fifty percent.

11. A method for a Raman generator, the method comprising:
passing a pump pulse through a Raman medium having a longitudinal central axis a plurality of times, each pass shifting at least a portion of the pump pulse energy or power into a Stokes-shifted pulse at a second wavelength; and
passing the Stokes-shifted pulse through the Raman medium a plurality of times to increase a power of the Stokes-shifted pulse;
wherein each pass of the pulses through the Raman medium follows a path;
wherein each path is one of parallel or anti-parallel to the other paths; and
wherein the paths of three or more consecutive passes of the pulses through the Raman medium alternate between opposite sides of the longitudinal central axis of the Raman medium.

12. The method of claim 11 , wherein passing the pulses through the Raman medium a plurality of times further comprises:
passing the pulses along multiple common paths through the Raman medium to increase a power of the Stokes-shifted pulse.

13. The method of claim 11 , wherein the conversion efficiency of a Raman generator performing the method determined by comparing the pump pulse initially received at the first wavelength to the generated Stokes-shifted pulse at the second wavelength after several passes through the Raman medium is greater than or equal to fifty percent.

14. The method of claim 11 , further comprising:
limiting diffractive spreading of the pump pulse and the Stoke-shifted pulse.

15. The method of claim 11 , wherein the passing of the pump pulse and the Stokes-shifted pulse through the Raman medium a plurality of times is carried out with two prisms of different size.

16. The method of claim 11 , wherein the pump pulse and the Stokes-shifted pulse are passed through two lenses and two prism-lens combinations, a prism portion of the prism-lens combinations passing both the pump pulse and the Stokes-shifted pulse more than two times through the Raman medium, and a lens portion of the prism-lens combinations and the two lenses limiting the diffractive spreading of the pump and Stokes-shifted pulse.

17. The method of claim 11 , wherein the Raman generator is configured such that the optical path and polarizations of the pump pulse and Stokes-shifted pulse are matched to preferred crystal axes in the Raman medium.

18. The method of claim 11 , wherein the Raman generator provides an optical length of one meter in a package having a maximum dimension of thirty centimeters.

19. The method of claim 11 , wherein the pump pulse and the Stokes-shifted pulse are passed through the Raman medium at least nine times.

20. The method of claim 11 , further comprising:
limiting a frequency spread of the Stokes-shifted beam relative to the frequency of the pump pulse.

21. The Raman generator of claim 1 , wherein the longitudinal central axis of the Raman medium denotes a longest dimension of the Raman medium.

Assignees

• Rockwell David A
• Shkunov Vladimir V
• Raytheon Co

Inventors

• Rockwell David A
• Shkunov Vladimir V

Classifications

• H01S3/094026

  for synchronously pumping, e.g. for mode locking · CPC title

• H01S3/2325

  Multi-pass amplifiers, e.g. regenerative amplifiers · CPC title

• H01S3/30 Primary

  using scattering effects, e.g. stimulated Brillouin or Raman effects · CPC title

• H01S3/083

  Ring lasers {(fibre ring lasers H01S3/06791)} · CPC title