Generation of high energy mid-infrared continuum laser pulses

Patent metadata

Field	Value
Publication number	US-10474002-B2
Application number	US-201615738522-A
Country	US
Kind code	B2
Filing date	Jun 27, 2016
Priority date	Jun 25, 2015
Publication date	Nov 12, 2019
Grant date	Nov 12, 2019

Abstract

In one aspect, a method is provided for generating supercontinuum laser pulses within a continuous mid-infrared spectral range in a chalcogenide material. This method includes focusing an input laser beam of femtosecond pulses with a pulse energy higher than 10 microjoule along an optical path of the input laser beam; placing a chalcogenide material at a selected location along the optical path of the laser beam so that the laser intensity at the chalcogenide material is sufficiently high to cause nonlinear optical absorption that causes conversion of input optical energy into supercontinuum laser pulses of a pulse energy at or above a microjoule level at optical wavelengths within a broad continuous mid-infrared spectral range without damaging the chalcogenide material; and simultaneously moving the chalcogenide material laterally relative to the input laser beam to avoid damage to the chalcogenide material.

First claim

What is claimed is:

1. A method for generating supercontinuum laser pulses within a continuous mid-infrared spectral range in a chalcogenide material, comprising:
focusing an input laser beam of femtosecond pulses with a pulse energy higher than 10 microjoule along an optical path of the input laser beam;
placing a chalcogenide material at a selected location along the optical path of the laser beam so that the laser intensity at the chalcogenide material is sufficiently high to cause nonlinear optical absorption that causes conversion of input optical energy into supercontinuum laser pulses of a pulse energy at or above a microjoule level at optical wavelengths within a broad continuous mid-infrared spectral range without damaging the chalcogenide material; and
simultaneously moving the chalcogenide material laterally relative to the input laser beam so that different portions of the chalcogenide material are exposed to the input laser beam at different times in exposing the chalcogenide material to the input laser beam in generating the supercontinuum laser pulses to avoid damage to the chalcogenide material.

2. The method as in claim 1 , wherein:
the chalcogenide material is a chalcogenide material glass.

3. The method as in claim 2 , wherein:
the chalcogenide glass material includes Ge and As.

4. The method as in claim 2 , wherein:
the chalcogenide material is a glass material that includes Ge and Se.

5. The method as in claim 2 , wherein:
the chalcogenide material is a glass material that includes As and Se.

6. The method as in claim 2 , wherein:
the chalcogenide glass material includes Ge, As, Se, Sb or Te.

7. The method as in claim 2 , wherein:
the chalcogenide glass material includes Ge 33 As 12 Se 55 , Ge 30 As 13 Se 32 Te 25 , Ge 10 As 40 Se 50 , Ge 28 Sb 12 Se 60 , or As 40 Se 60 .

8. The method as in claim 1 , wherein:
each laser pulse of the input laser beam has a pulse energy density greater than 100 GW/cm 2 and an input pulse energy of more than 10 microjoules.

9. The method as in claim 8 , wherein:
the chalcogenide material is placed at a location away from a focus of the laser beam along the optical path.

10. The method as in claim 8 , wherein:
the input laser beam is controlled at a laser wavelength greater than a cutoff laser wavelength that is shorter than 3800 nm, wherein input light at a laser wavelength shorter than the cutoff laser wavelength strongly absorbed to cause damage to the chalcogenide material.

11. The method as in claim 10 , wherein:
the input laser beam is controlled at a laser wavelength greater than a cutoff laser wavelength that is shorter than 3725 nm to avoid damage to the chalcogenide material caused by a high optical energy density of each laser pulse of the input laser beam.

12. The method as in claim 11 , wherein:
the input laser beam is controlled at a laser wavelength around 3725 nm.

13. The method as in claim 11 , wherein:
the input laser beam is controlled at a laser wavelength longer than 3725 nm.

14. The method as in claim 11 , wherein:
the input laser beam is controlled at a laser wavelength around 3725 nm.

15. The method as in claim 10 , wherein:
the input laser beam is at or near 4000 nm.

16. The method as in claim 10 , wherein:
the input laser beam is at or near 5000 nm.

17. The method as in claim 1 , wherein:
setting the energy of each laser pulse of the input laser beam at tens of microjoules when incident at the chalcogenide material; and
controlling an optical wavelength and each pulse energy density of the input laser beam generate the supercontinuum laser pulses at or above a 20 dB level in a continuous spectral range from about 2.5 microns to about 10 microns in wavelength.

18. A device for optical sensing based on supercontinuum laser pulses within a continuous mid-infrared spectral range in a chalcogenide material, comprising:
a laser source module that produces an input laser beam at an input laser wavelength of femtosecond pulses with a pulse energy higher than 10 microjoule;
an input beam focusing device in an optical path of the input laser beam to focus the input laser beam at a focus location to produce a high pulse energy density;
a motorized actuator that holds a chalcogenide material at a selected location along the optical path of the laser beam so that the laser intensity at the chalcogenide material is sufficiently high to cause nonlinear optical absorption that causes conversion of input optical energy into supercontinuum laser pulses of a pulse energy at or above a microjoule level at optical wavelengths within a broad continuous mid-infrared spectral range without damaging the chalcogenide material, the motorized actuator operable to move the chalcogenide material laterally relative to the input laser beam so that different portions of the chalcogenide material are exposed to the input laser beam at different times in exposing the chalcogenide material to the input laser beam in generating the supercontinuum laser pulses to avoid damage to the chalcogenide material; and
an output beam device in an optical path of the generated supercontinuum laser pulses to direct the generated supercontinuum laser pulses as an optical sensing beam to a target for optically sensing the target.

19. The device as in claim 18 , wherein:
the output beam device includes a parabola reflector that reflects and directs the generated supercontinuum laser pulses onto the target.

20. The device as in claim 18 , wherein:
the input beam focusing device includes a parabola reflector that reflects and focuses the input laser beam.

21. The device as in claim 18 , wherein:
the input beam focusing device includes a lens that focuses the input laser beam, and
the output beam device includes a parabola reflector that reflects and directs the generated supercontinuum laser pulses onto the target.

22. The device as in claim 18 , wherein:
the laser source module includes an optical amplifier to produce amplified laser pulses and an optical parametric amplifier that receives the amplified laser pulses to produce the input laser beam having femtosecond pulses at the input laser wavelength and a pulse energy higher than 10 microjoule.

23. The device as in claim 18 , wherein:
the motorized actuator is operable to move the chalcogenide material laterally along two directions.

24. The device as in claim 18 , wherein:
the motorized actuator is configured to hold the chalcogenide material at a position away from a focus of the input laser beam produced by the input beam focusing device.

25. The device as in claim 18 , further comprising:
an optical detector that receives light from the target under illumination of the generated supercontinuum laser pulses to provide optical sensing information on the target.

26. The device as in claim 18 , wherein:
the chalcogenide material includes Ge 33 As 12 Se 55 , Ge 30 As 13 Se 32 Te 25 , Ge 10 As 40 Se 50 , Ge 28 Sb 12 Se 60 , or As 40 Se 60 .

Assignees

• Univ Cornell

Inventors

• Petersen Poul B
• Stingel Ashley

Classifications

• G01N21/35

  using infrared light (G01N21/39 takes precedence) · CPC title

• G02F1/39

  for parametric generation or amplification of light, infrared or ultraviolet waves · 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

• G02F1/3501

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

• G02F1/3555

  Glasses · CPC title