Supercontinuum light source

Patent metadata

Field	Value
Publication number	US-9986904-B2
Application number	US-201615283437-A
Country	US
Kind code	B2
Filing date	Oct 2, 2016
Priority date	Jun 1, 2012
Publication date	Jun 5, 2018
Grant date	Jun 5, 2018

Abstract

A supercontinuum light source can comprise a seed laser arranged to provide seed pulses with a pulse frequency F seed ; a pulse frequency multiplier (PFM) arranged to multiply the seed pulses by converting pulses having the pulse frequency F seed to pump pulses with a pulse frequency F pump , where F pump is larger than F seed ; and a non-linear element arranged to receive said pump pulses and convert said pump pulses to pulses of supercontinuum light. The PFM can further comprise a splitter for splitting pulses into first and second sub beams each having the same pulse frequency, where the PFM is configured such that the sub beams experience different delays; and a combiner for combining said first and second sub beams into a beam having the pulse frequency that is greater than said same pulse frequency. The splitter can have an uneven splitter ratio. The disclosure includes other embodiments as well.

First claim

The invention claimed is:

1. A supercontinuum light source comprising:
a seed laser arranged to provide seed pulses with a pulse frequency F seed ;
a pulse frequency multiplier (PFM) arranged to multiply the seed pulses by converting pulses having a pulse frequency of F seed to pump pulses with a pulse frequency F pump , where F pump is larger than F seed ;
a non-linear element arranged to receive said pump pulses and convert said pump pulses to pulses of supercontinuum light;
wherein said PFM further comprises
a splitter for splitting seed pulses into first and second sub beams each having a pulse frequency F seed , said PFM configured such that one of said sub beams is delayed relative to the other of said sub beams;
another splitter for splitting out further sub beams each having a pulse frequency that is greater than F seed and less than F pump , said PFM configured such that one of said further sub beams is delayed relative to the other of said further sub beams; and
a combiner for combining the further sub beams into a beam having the pulse frequency F pump ; and

wherein said seed laser is arranged to provide seed pulses with a pulse duration t seed that is longer than about 1 ps.

2. The supercontinuum light source of claim 1 wherein said seed pulses have a pulse duration t seed that is shorter than about 50 ps.

3. The supercontinuum light source of claim 1 wherein said seed laser comprises a mode locked Yb laser.

4. The supercontinuum light source of claim 3 wherein said mode locked Yb laser comprises a fiber laser that is passively mode locked via a SESAM (Semiconductor Saturable Absorber Mirror).

5. The supercontinuum light source of claim 1 wherein said PFM comprises a delay line for delaying one of the first and second sub beams.

6. The supercontinuum light source of claim 1 wherein said PFM comprises an attenuator for attenuating a sub beam.

7. The supercontinuum light source of claim 6 wherein one of said splitters has a splitter ratio that is uneven.

8. The supercontinuum light source of claim 1 wherein one of said splitters has a splitter ratio that is uneven.

9. The supercontinuum light source of claim 1 comprising first and second amplifiers and wherein said PFM is located between the amplifiers.

10. The supercontinuum light source of claim 1 wherein F pump is 150 MHz or more.

11. The supercontinuum light source of claim 1 wherein said non-linear element comprises a microstructured optical fiber.

12. The supercontinuum light source of claim 1 wherein said another splitter comprises a coupler that combines said sub beams and that splits said combined sub beams into said further sub beams.

13. The supercontinuum light source of claim 1 wherein the light source is configured such that the pulses of supercontinuum light have a pulse duration and wherein average optical power output from the supercontinuum lights source is less than 5 Watt output per ps pulse duration.

14. A supercontinuum light source comprising:
a seed laser arranged to provide seed pulses with a pulse frequency F seed ;
a pulse frequency multiplier (PFM) arranged to multiply the seed pulses by converting pulses having a pulse frequency of F seed to pump pulses with a pulse frequency F pump , where F pump is larger than F seed ;
a non-linear element arranged to receive said pump pulses and convert said pump pulses to pulses of supercontinuum light; and
wherein said PFM further comprises
a splitter for splitting seed pulses into first and second sub beams each having the same pulse frequency, said PFM configured such that said sub beams experience different delays;
a combiner for combining sub beams into a beam having a pulse frequency that is greater than said same pulse frequency; and
an attenuator for attenuating the first sub beam such that said combiner combines the second sub beam with an attenuated first sub beam into said beam having said pulse frequency that is greater than the pulse frequency.

15. The supercontinuum light source of claim 14 wherein said splitter has an uneven splitter ratio.

16. The supercontinuum light source of claim 14 wherein said seed laser is arranged to provide seed pulses with a pulse duration t seed that is longer than about 1 ps.

17. The supercontinuum light source of claim 14 wherein said seed laser comprises a mode locked Yb fiber laser.

18. The supercontinuum light source of claim 14 wherein the pulses of supercontinuum light have a pulse duration and wherein the supercontinuum light source is configured such that the average optical power output from the supercontinuum light source is less than 5 Watts per ps pulse duration.

19. The supercontinuum light source of claim 14 wherein the supercontinuum light source is configured such that the total average optical power in the range 400 nm-850 nm is less than 100 mW.

20. A supercontinuum light source comprising:
a seed laser arranged to provide seed pulses with a pulse frequency F seed ;
a pulse frequency multiplier (PFM) arranged to multiply the seed pulses by converting pulses having a pulse frequency of F seed to pump pulses with a pulse frequency F pump , where F pump is larger than F seed ;
a non-linear element arranged to receive said pump pulses and convert said pump pulses to pulses of supercontinuum light;
wherein said PFM further comprises
a splitter for splitting seed pulses into first and second sub beams each having a pulse frequency F seed , said PFM configured such that said sub beams experience different delays;
a coupler for combining sub beams and splitting the combined sub beams into further sub beams each having said pulse frequency that is greater than F seed and less than F pump , said PFM configured such that said further sub beams experience different delays; and
a combiner for combining said further sub beams into a beam having the pulse frequency F ummp .

21. The supercontinuum light source of claim 20 wherein said seed laser comprises a mode locked Yb laser.

22. The supercontinuum light source of claim 21 wherein said mode locked Yb laser comprises a fiber laser that is passively mode locked via a SESAM.

23. A supercontinuum light source comprising:
a seed laser arranged to provide seed pulses with a pulse frequency F seed ;
a pulse frequency multiplier (PFM) arranged to multiply the seed pulses by converting pulses having the pulse frequency F seed to pump pulses with a pulse frequency F pump , where F pump is larger than F seed ;
a non-linear element arranged to receive said pump pulses and convert said pump pulses to pulses of supercontinuum light; and
wherein said PFM further comprises
a splitter for splitting pulses into first and second sub beams each having the same pulse frequency, said PFM configured such that said sub beams experience different delays;
a combiner for combining said first and second sub beams into a beam having the pulse frequency that is greater than said same pulse frequency; and
wherein said splitter has a splitter ratio and wherein said splitter ratio is uneven.

24. The supercontinuum light source of claim 23 wherein said PFM comprises a second splitter, said second splitter having a splitter ratio that is uneven.

Assignees

• Nkt Photonics As

Inventors

• Thomsen Carsten L
• Andersen Thomas Vestergaard
• Feuchter Thomas

Classifications

• G02F1/35 Primary

  Non-linear optics · CPC title

• G02F1/365

  in an optical waveguide structure (G02F1/377, {G02F1/395} take precedence) · CPC title

• H01S5/0657

  Mode locking, i.e. generation of pulses at a frequency corresponding to a roundtrip in the cavity · CPC title

• G02F1/353

  Frequency conversion, i.e. wherein a light beam is generated with frequency components different from those of the incident light beams · CPC title

• H01S5/0092

  for nonlinear frequency conversion, e.g. second harmonic generation [SHG] or sum- or difference-frequency generation outside the laser cavity · CPC title