Systems and methods for lasing from a molecular gas

Patent metadata

Field	Value
Publication number	US-9166358-B2
Application number	US-201213546888-A
Country	US
Kind code	B2
Filing date	Jul 11, 2012
Priority date	Jul 11, 2011
Publication date	Oct 20, 2015
Grant date	Oct 20, 2015

Abstract

Systems and methods for lasing molecular gases, and systems and methods of detecting molecular species are provided. The systems and methods can include the use of an excitation laser tuned to a wavelength associated with oxygen or nitrogen. The lasing can occur in both the forward and reverse directions relative to the excitation laser beam. Reverse lasing can provide a laser beam that propagates back toward the excitation laser source, and can provide a method for remote sampling of molecular species contained in the air. For example, systems and methods of detecting a molecular species of interest can be achieved by using the properties of the backward or forward propagating air laser to indicate a change in a pulse from the source of laser pulses caused by a modulation laser tuned to interact with the molecular species of interest.

First claim

What is claimed is:

1. A method for lasing in air without a resonating cavity, the method comprising:
using a source of laser pulses to dissociate at least one molecular species comprising atomic constituents into the atomic constituents; and
using the source of laser pulses to excite at least one of the dissociated atomic constituents by at least two-photon absorption to an energy level that forms a population inversion along an excitation path of an upper lasing level to produce a gain path for amplified stimulated emission of radiation.

2. The method of claim 1 , wherein the source of laser pulses comprises a first laser and a second laser, the first laser configured to generate a first laser pulse to dissociate the at least one molecular species, and the second laser configured to generate a second laser pulse to excite the at least one of the dissociated atomic constituents.

3. The method of claim 1 , wherein the source of laser pulses comprises a laser configured to generate a plurality of laser pulses, each laser pulse interacting with both the at least one molecular species and the at least one dissociated atomic constituent, the interaction with the at least one molecular species dissociating the at least one molecular species and the interaction with the at least one dissociated atomic constituent exciting the at least one dissociated atomic constituent.

4. The method of claim 1 , wherein the at least one molecular species is selected from the set of: molecular oxygen and molecular nitrogen.

5. The method of claim 1 , wherein the gain path is in both a forward direction and a reverse direction along the excitation path, leading to air laser beams propagating in both the forward direction and the reverse direction.

6. The method of claim 5 , wherein the air laser beam propagating in the reverse direction is amplified by subsequent dissociation and pumping of at least one of the atomic constituents at a location and a time coinciding with a backward propagating air laser pulse.

7. The method of claim 1 , further comprising detecting a specific molecular species.

8. A method of detecting molecular species in air, the method comprising:
using a source of laser pulses to dissociate at least one molecular species comprising atomic constituents into the atomic constituents;
using the source of laser pulses to excite at least one of the dissociated atomic constituents by at least two photon absorption to form a population inversion along an excitation path of an upper lasing level to produce a gain path for amplified stimulated emission of radiation for lasing in air without a resonating cavity; and
employing stimulated Raman scattering effects;
wherein the gain path is in both a forward direction and in a reverse direction along the excitation path, leading to air laser beams propagating in both the forward direction and the reverse direction;
wherein at least one air laser beam interacts with a specific molecular species in the excitation laser path, the interaction producing Raman shifted sidebands comprising wavelengths; and
wherein the wavelengths are indicative of the specific molecular species.

9. The method of claim 8 , wherein the source of laser pulses comprises a first laser and a second laser, the first laser configured to generate a first laser pulse to dissociate the at least one molecular species, and the second laser configured to generate a second laser pulse to excite the at least one of the dissociated atomic constituents.

10. The method of claim 8 , wherein the source of laser pulses comprises a laser configured to generate a plurality of laser pulses, each laser pulse interacting with both the at least one molecular species and the at least one dissociated atomic constituent, the interaction with the at least one molecular species dissociating the at least one molecular species and the interaction with the at least one dissociated atomic constituent exciting the at least one dissociated atomic constituent.

11. The method of claim 8 , wherein the at least one molecular species is selected from the set of: molecular oxygen and molecular nitrogen.

12. A system for lasing a molecular gas in air without a resonating cavity comprising:
a source of laser pulses configured to dissociate at least one molecular species comprising atomic constituents into the atomic constituents;
wherein the source of laser pulses is also configured to excite at least one of the dissociated atomic constituents by at least two-photon absorption to form a population inversion along an excitation path of an upper lasing level to produce a gain path for amplified stimulated emission of radiation.

13. The system of claim 12 , wherein the source of laser pulses comprises a first laser and a second laser, the first laser configured to generate a first laser pulse to dissociate the at least one molecular species, and the second laser configured to generate a second laser pulse to excite the at least one of the dissociated atomic constituents.

14. The system of claim 12 , wherein the source of laser pulses comprises a laser configured to generate a plurality of laser pulses, each laser pulse interacting with both the at least one molecular species and the at least one dissociated atomic constituent, the interaction with the at least one molecular species dissociating the at least one molecular species and the interaction with the at least one dissociated atomic constituent exciting the at least one dissociated atomic constituent.

15. The system of claim 12 , wherein the at least one molecular species is selected from the set of: molecular oxygen and molecular nitrogen.

16. The system of claim 12 , wherein the gain path is in both a forward direction and a reverse direction along the excitation path, leading to air laser beams propagating in both the forward direction and the reverse direction.

17. The system of claim 16 , wherein the air laser beam propagating in the reverse direction is amplified by subsequent dissociation and pumping of at least one of the atomic constituents at a location and a time coinciding with a backward propagating laser pulse.

18. A method of detecting molecular species in air, the method comprising:
using a source of laser pulses to dissociate at least one molecular species comprising atomic constituents into the atomic constituents;
using the source of laser pulses to excite at least one of the dissociated atomic constituents by at least two-photon absorption to form a population inversion along an excitation path of an upper lasing level to produce a gain path for amplified stimulated emission of radiation for lasing in air without a resonating cavity;
using a modulation laser to generate a modulation beam configured to co-propagate with a beam from the source of laser pulses along the excitation path; and
determining whether the co-propagating modulation beam alters a property of a reverse-propagating air laser beam;
wherein the gain path is at least in a reverse direction along the excitation path, leading to the reverse-propagating air laser beam;
wherein the modulation beam is configured to transfer energy to a specific molecular species such that the energized specific molecular species alters an index of refraction of air in the excitation laser path.

19. The method of claim 18 , wherein the source of laser pulses comprises a first laser and a second laser, the first laser configured to generate a first laser pulse to dissociate the at least one molecular species, and the second laser configured to generate a

Assignees

• Miles Richard B
• Dogariu Arthur
• Michael James B
• Univ Princeton

Inventors

• Miles Richard B
• Dogariu Arthur
• Michael James B

Classifications

• H01S3/0014

  Monitoring arrangements not otherwise provided for (photometry G01J1/00, e.g. G01J1/4257; radiation pyrometry G01J5/00; measuring coherence of light G01J9/00; measuring wavelength of light G01J9/00, e.g. G01J9/0246; measuring optical pulses G01J11/00; calorimetrically measuring power of laser beams G01K17/003) · CPC title

• G01N21/65

  Raman scattering · CPC title

• G01N21/1717 Primary

  with a modulation of one or more physical properties of the sample during the optical investigation, e.g. electro-reflectance · CPC title

• H01S3/2391

  emitting at different wavelengths · CPC title

• G01N2021/1793

  Remote sensing · CPC title