Range gated remote measurement utilizing two-photon absorption

• US 6,384,903 B1
• Filed: 02/28/1977
• Issued: 05/07/2002
• Est. Priority Date: 02/28/1977
• Status: Expired due to Term

• Current Assignee: BAE Systems Information and Electronic Systems Integration Incorporated (BAE Systems Plc)
• Original Assignee: BAE Systems Information and Electronic Systems Integration Incorporated (BAE Systems Plc)
• Inventors: Fuller, Harrison W.
• Primary Examiner(s): Buczinski, Stephen C.
• Application Number:
  US05/773,636
• Time in Patent Office: 9,199 Days
• Field of Search: 324/0.5 E, 324/0.5 F, 324/43.L, 356/114, 356/119, 356/5, 356/103, 356/201, 356/4.01, 356/5.01, 356/5.1, 356/438, 356/301, 356/342
• US Class Current: 356/4.01
• CPC Class Codes: G01J 3/42 Absorption spectrometry; Double beam spectrometry; Flicker spectrometry; Reflection spectrometry beam switching arrangements G01J3/08

Abstract

Two-photon absorption measurements are made at various points remote from monitoring apparatus by apparatus which includes two lasers that produce counter-propagating beams through the earth'"'"'s atmosphere. The lasers are tuned such that the sum of the energies of the photons in each of the laser beams equals that associated with a predetermined transition of a gas in the earth'"'"'s atmosphere. In one embodiment, a pulsed laser and a CW laser are used. The pulse from the pulsed laser propagates along the CW beam produced by the CW laser and overlaps the CW beam at positions determined by a range gating technique, which makes possible the measurement of the two photon absorption at the various positions of overlap or coincidence. In one embodiment, the subject apparatus is utilized for pollution monitoring, in which the frequencies of the lasers are tuned such that the energies of the photons from these lasers add up to a transition of a predetermined pollutant.

Claims

1. Apparatus for making remote atomic absorption measurements comprising:

means, including two collimated counter-propagating beams of coherent energy, for establishing two-photon absorption in the earth'"'"'s atmosphere at a number of selectable locations along the direction of said beams, and,

means for measuring a two-photon absorption related characteristic of one of said beams after said one beam has participated in establishing two-photon absorption at a selected location.

2. The apparatus of claim 1 wherein said measuring means includes means for correlating the measured absorption related characteristic with the particular location selected.

3. The apparatus of claim 2 wherein said correlating means includes means for measuring the range of the two-photon absorption at a selected location.

4. The apparatus of claim 1 wherein one of said beams is pulsed and the other of said beams is CW, said means for establishing two-photon absorption including means for sending out said pulse along said CW beam, with the points of coincidence and overlap of said pulse and CW beam defining the selected location of the two-photon absorption, said measuring means including means for detecting said absorption related characteristic as a function of the location of said pulse.

5. The apparatus of claim 4 wherein said detecting means includes means for determining the range of said pulse by establishing the time that said pulse is at a predetermined location and the times that said absorption related characteristic is measured at a location of known position relative to said predetermined location.

6. The apparatus of claim 1 wherein each of said beams is produced by a source of coherent radiation, said sources being spaced apart and aimed at each other to produce said counter-propagating beams.

7. The apparatus of claim 1 wherein each of said beams is produced by a source of coherent radiation, said sources being located at one location and further including retroflective means at a second location spaced from said one location, said sources being aimed at said retroflective means.

8. The apparatus of claim 7 wherein one of said sources is a pulsed source and the other of said sources is a CW source, said means for establishing said two-photon absorption further including means for actuating said pulsed source prior to actuating said CW source, with the points of coincidence and overlap of said outgoing CW beam and the retroflected pulse defining the location of the two-photon absorption.

9. The apparatus of claim 8 wherein said measuring means includes means for detecting said absorption-related characteristic as a function of the location of said pulse.

10. The apparatus of claim 9 wherein said detecting means measures the location of said pulse as a function of its range from said retroflecting means.

11. The apparatus of claim 9 wherein said detecting means includes means for establishing the time said pulse is at a predetermined location and times that said absorption related characteristic is measured at a location of known position relative to said predetermined location.

12. The apparatus of claim 1 wherein said means for establishing two-photon absorption includes two sources of coherent electromagnetic energy, the photon energies of which add up to that associated with a transition of a predetermined gas, and means for varying the location at which said energies add up to that of said transition.

13. The apparatus of claim 12 and further including means for establishing a third beam of electromagnetic energy colinear with said counter-propagating beams, said third beam being of a frequency and a corresponding photon energy which does not interfere with the measurement of said two-photon absorption-related characteristic, and means for normalizing the measurement of the two-photon absorption-related characteristic with respect to a characteristic of said third beam.

14. The apparatus of claim 13 wherein the two-photon absorption is measured by the intensity of said one beam after the two-photon interaction and wherein said normalizing means includes means for subtracting the measured intensity of said one beam from that of said third beam.

15. The apparatus of claim 1 wherein said one beam is linearly polarized and wherein said measuring means includes linear polarizer means cross polarized with respect to the direction of linear polarization of said one beam, means for directing said one beam through said linear polarizer means after it has participated in establishing the two-photon absorption, and means for detecting the intensity of said one beam after it has passed through said linear polarizer means.

16. The apparatus of claim 1 wherein the other of said beams is in the form of a pulse of energy which propagates along said one beam such that two-photon absorption takes place at the successive locations of overlap of the pulse and said one beam.

17. The apparatus of claim 16 wherein said measuring means includes means for measuring the intensity of said one beam as a function of the locations of overlap between said pulse and said one beam, thereby to establish two-photon absorption at said selected locations.

18. The apparatus of claim 17 and further including means for generating a reference beam, the intensity of which correlating, location by location, to the attenuations over the path of said other beams due to attenuation modes other than two-photon absorption, and means for normalizing said one beam with respect to said reference beam on a location by location basis.

19. Apparatus for making remote atomic absorption measurement comprising:

means, including two collimated counter-propagating beams of coherent energy, for establishing two-photon absorption in the earth'"'"'s atmosphere at selected locations,

means for producing stimulated emission at the locations of two-photon absorption, and,

means for measuring said stimulated emission at said selected locations.

20. The apparatus of claim 19 wherein said means for producing said stimulated emission includes means for generating a beam of coherent energy colinear with said counter-propagating beams.

21. The apparatus of claim 20 wherein said colinear beam is at a frequency corresponding to a predetermined transition of an element in the earth'"'"'s atmosphere different from that at which said two-photon absorption takes place.

22. Apparatus for measuring atomic absorption associated with atoms or molecules of a gas comprising:

means, including two collimated counter-propagating beams of coherent energy, for establishing two-photon absorption in said gas, and,

means for measuring a two-photon absorption related characteristic of one of said beams after said one beam has participated in establishing two-photon absorption.

23. The apparatus of claim 22 wherein said one beam is linearly polarized and wherein said measuring means includes crossed polarizer detection means.

24. The apparatus of claim 22 wherein said means for establishing said counter-propagating beams includes means for linearly polarizing said one beam prior to the two-photon interaction, and wherein said measuring means includes detector means illuminated by said one beam after it has participated in establishing the two-photon absorption, and linear polarizing means crossed with respect to said first mentioned linear polarizing means, said crossed linear polarizing means being positioned such that said one beam passes through it after said one beam has participated in establishing the two-photon absorption prior to detection.

25. The apparatus of claim 22 wherein said measuring means includes means for normalizing the measurement made thereby to a circularly polarized component of said one beam which does not contribute to the two-photon absorption.

26. The apparatus of claim 25 wherein said normalizing means includes crossed polarizing means.

27. The apparatus of claim 25 wherein said normalizing means includes means for resolving RHCP and LHCP components of said one beam and subtracting one from the other.

28. Apparatus for measuring atomic absorption associated with atoms or molecules of a gas comprising:

means, including two collimated counter-propagating beams of coherent energy, one of said beams being linearly polarized, for establishing absorption in said gas, and,

means including crossed polarizer detection means for measuring an absorption related characteristic of said linearly polarized beam after said linearly polarized beam has participated in establishing said absorption.

29. Apparatus for measuring atomic absorption associated with atoms or molecules of an unconfined gas in the earth'"'"'s atmosphere comprising:

means, including two counter-propagating beams of coherent energy for establishing absorption in said unconfined gas, and,

means for measuring an absorption related characteristic of one of said beams after said one beam has participated in establishing said absorption.

30. The apparatus of claim 29 wherein said one beam is linearly polarized and wherein said measuring means includes crossed polarizer detection means.