Supercontinuum generation apparatus and method

Patent metadata

Field	Value
Publication number	US-9971229-B2
Application number	US-201615262725-A
Country	US
Kind code	B2
Filing date	Sep 12, 2016
Priority date	Sep 17, 2015
Publication date	May 15, 2018
Grant date	May 15, 2018

Abstract

Apparatuses and methods for supercontinuum generation using a laser beam and a plurality of condensed state transparent plates are presented. As an example, plate material to be used for one of the plurality of plates is determined. A thickness of the one of the plurality of plates is also determined. An allowable laser intensity of the laser beam is then determined to be λ/(2n 0 n 2 L), where λ is the central incident wavelength in vacuum, n 0 is the linear refractive index, n 2 is the third-order nonlinear coefficient. A location of a next plate is then determined to be a distance downstream from the one of the plurality of plates where a laser intensity of the laser beam returns to a value of the determined allowable laser intensity.

First claim

The invention claimed is:

1. A continuous spectrum generation apparatus, comprising:
a laser light source configured to emit a laser beam;
a plurality of condensed state transparent plates, disposed in sequence on a transmitting path of the laser beam to successively and sequentially extend a spectral bandwidth of the laser beam, wherein one or more of temporal, spatial and spectral value of a pulse of the laser beam in a forward propagation direction z through a plate number n are determined as a function of z;
a pulse characterization apparatus configured to characterize the pulse of the laser beam; and
wherein a spacing between two of the plurality of plates is determined by where an intensity of the laser beam is λ/(2n 0 n 2 L), where λ is the central incident wavelength in vacuum, n 0 is the linear refractive index, n 2 is the third-order nonlinear coefficient, L is the thickness of the plates.

2. The apparatus of claim 1 wherein spacing between two of the plurality of plates is determined by where an intensity of the laser beam is less than 0.9 times a damage intensity of a generating medium.

3. The apparatus of claim 1 wherein spacing between two of the plurality of plates is determined by where an intensity of the laser beam is less than 0.6 times a damage intensity of a generating medium.

4. The apparatus of claim 1 wherein n 2 is a Kerr coefficient.

5. The apparatus of claim 1 wherein duration of the pulse of the laser beam is below 70 femtoseconds.

6. The apparatus of claim 1 wherein duration of the pulse of the laser beam is below 50 femtoseconds.

7. The apparatus of claim 1 wherein the plurality of condensed state transparent plates broaden the spectral value of the pulse of the laser beam to a range of 100-2000 nm.

8. The apparatus of claim 1 wherein the pulse characterization apparatus comprises an optical spectrometer and a frequency-resolved optical gating arrangement to measure the pulse duration between 3 fs to 1000 fs.

9. The apparatus of claim 1 wherein the pulse duration of the laser beam is below 500 femtoseconds.

10. The apparatus of claim 1 wherein the plurality of condensed state transparent plates broaden the spectral value of the pulse of the laser beam to a range of 30-85 nm.

11. The apparatus of claim 1 further comprising another set of a plurality of condensed state transparent plates concatenated to the plurality of plates of claim 1 .

12. The apparatus of claim 11 further comprising a pulse compressor inserted between the two sets of plurality of condensed state transparent plates.

13. The apparatus of claim 1 further comprising a broad bandwidth quarter-wave plate configured to convert the emitted laser beam from the laser light source from a linearly polarized to a circularly polarized laser beam.

14. The apparatus of claim 13 wherein the broadband quarter-wave plate has an effective wavelength bandwidth in the range of 100-150 nm.

15. The apparatus of claim 1 wherein the plurality of plates are optically polished.

16. The apparatus of claim 1 further comprising a pulse compressor configured to shorten the supercontinuum pulse outputted from the plurality of condensed state transparent plates.

17. A method for supercontinuum generation using a laser beam and a plurality of condensed state transparent plates, comprising:
determining plate material to be used for one of the plurality of plates;
determining a thickness of the one of the plurality of plates; and
determining an allowable laser intensity of the laser beam to be λ/(2n 0 n 2 L), where λ is the central incident wavelength in vacuum, n 0 is the linear refractive index, n 2 is the third-order nonlinear coefficient; and
determining a location of a next plate be a distance downstream from the one of the plurality of plates where a laser intensity of the laser beam returns to a value of the determined allowable laser intensity.

18. The method of claim 17 wherein n 2 is the Kerr coefficient.

19. The method of claim 17 wherein the laser beam is pulsing below 70 femtoseconds.

20. The method of claim 17 wherein the laser beam is pulsing below 50 femtoseconds.

21. The method of claim 17 wherein the plurality of condensed state transparent plates broaden the spectral value of the laser beam to a range of 100-2000 nm.

22. The method of claim 17 wherein the pulse duration of the laser beam is below 500 femtoseconds.

23. The method of claim 17 wherein the plurality of condensed state transparent plates broaden the spectral value of the pulse of the laser beam to a range of 30-85 nm.

24. The method of claim 17 further comprising another set of a plurality of condensed state transparent plates concatenated to the plurality of plates of claim 17 .

25. The method of claim 24 further comprising a pulse compressor inserted between the two sets of plurality of condensed state transparent plates.

26. The method of claim 17 further comprising providing a broad bandwidth quarter-wave plate configured to convert the emitted laser beam from the laser light source from a linearly polarized to a circularly polarized laser beam.

27. The method of claim 26 wherein the broadband quarter-wave plate has an effective wavelength bandwidth in the range of 100-150 nm.

28. The method of claim 17 wherein the plurality of plates are optically polished.

Assignees

• Academia Sinica

Inventors

• Kung Andrew Hing Cheong
• Cheng Yu-Chen
• Lu Chih-Hsuan

Classifications

• H01S2301/08

  Generation of pulses with special temporal shape or frequency spectrum · CPC title

• G02F1/353 Primary

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

• H01S3/0092

  Nonlinear frequency conversion, e.g. second harmonic generation [SHG] or sum- or difference-frequency generation outside the laser cavity (nonlinear frequency conversion per se G02F1/35) · CPC title

• G02F1/3555

  Glasses · CPC title

• G02F1/3501 Primary

  Constructional details or arrangements of non-linear optical devices, e.g. shape of non-linear crystals · CPC title