COVERT ILLUMINATION

• US 20100148093A1
• Filed: 05/13/2008
• Published: 06/17/2010
• Est. Priority Date: 05/14/2007
• Status: Abandoned Application

• Current Assignee: Qinetiq Limited (QinetiQ Group PLC)
• Original Assignee: Qinetiq Limited (QinetiQ Group PLC)
• Inventors: Benton, David Mark
• Application Number:
  US12/451,480
• Publication Number:
  US 20100148093A1
• Time in Patent Office: Days
• US Class Current: 250/492.100
• CPC Class Codes: G01S 17/02 Systems using the reflection of electromagnetic waves other than radio waves G01S17/66 takes precedence
• CPC Class Codes: G01S 17/18 wherein range gates are used
• CPC Class Codes: G01S 7/4814 of transmitters alone
• CPC Class Codes: G02B 23/12 with means for image conversion or intensification

Abstract

This invention relates to methods and apparatus for covert illumination. The method involves illuminating the scene with light which is tuned to an absorption resonances of atmospheric oxygen gas. Light tuned to have a wavelength corresponding to an oxygen absorption wavelength travelling through the atmosphere is therefore attenuated by absorption. The method therefore teaches that a low power illumination source can be used to illuminate nearby objects, thus allowing the detail thereof to be resolved, and the illuminating light reflected from the object, or even the light source itself, will be undetectable beyond a certain range due to atmospheric absorption. The illumination may be used in conjunction with the use of low light level imagers to image a scene. Alternatively the illumination could be used for short range optical communication which will be undetectable at much longer range.

Claims

1. A method of covert illumination comprising providing an optical source having an optical output tuned to an absorption wavelength of atmospheric oxygen, and illuminating the scene with said optical source.

2. A method according to claim 1 wherein the absorption wavelength of atmospheric oxygen corresponds to an absorption resonance of oxygen gas at wavelengths around 760 nm.

3. A method according to claim 1 wherein the atmospheric absorption wavelength is outside the visible spectrum.

4. A method as claimed in claim 1 wherein the power of the source is of the order of, or less than 1 milliwatt.

5. A method as claimed in claim 1 further comprising the step of controlling the divergence of the source so that only limited viewing directions could see the source directly.

6. A method as claimed in claim 1 wherein the optical source comprises a laser.

7. A method according to claim 1 further comprising the step of maintaining the wavelength of the source at the desired absorption wavelength.

8. A method according to claim 7 where in the step of maintaining the wavelength of the source comprising passing at least some of the output through a known sample which absorbs at the absorption wavelength of atmospheric oxygen, monitoring the level of absorption and applying feedback to the source to keep the wavelength at the peak of the absorption.

9. A method according to claim 8 wherein the known sample is provided in one or more photonic bandgap fibres capable of transmitting light at the absorption wavelength of atmospheric oxygen.

10. A method according to claim 1 wherein the absorption wavelength of atmospheric oxygen is substantially at or near the wavelength of peak response of a low light level imager.

11. A method according to claim 1 further comprising imaging the illuminated scene with a low light level imager.

12. A method according to claim 11 wherein the low light level imager is an intensified CCD imager.

14. A method as claimed in claim 1 wherein the optical output of the source is pulsed.

15. A method as claimed in claim 14 wherein the pulse timing is arranged to be synchronous with image acquisition of a gated low light level imager.

16. A method according to claim 1 further comprising the step of modulating the optical output with a data encoding.

18. A method according to claim 16 wherein the modulated output is transmitted through the atmosphere to a receiver comprising a high speed detector and a processor capable of decoding the modulation.

13. (canceled)

17. (canceled)

19. A method of covert low light level imaging comprising illuminating a scene with an optical source having an optical output tuned an absorption wavelength of atmospheric oxygen and imaging the scene with a low light level imager responsive to the wavelength of illumination.

20. (canceled)

21. An optical source tuned to an atmospheric absorption wavelength comprising a laser having a feedback control means for wavelength locking the laser output to the atmospheric absorption wavelength, wherein the feedback control means passes at least some of the laser output through a sample of the target atmospheric constituent and analyses the intensity thereof and wherein the target atmospheric constituent is held within a photonic bandgap fibre which is transmissive at the atmospheric absorption wavelength.

22. An optical source as claimed in claim 21 arranged such that all of the laser output passes through the photonic bandgap fibre and further comprising means for directing part of the radiation exiting the photonic bandgap fibre to a detector.

23. An optical source as claimed in claim 21 wherein the atmospheric absorption wavelength corresponds to an absorption of oxygen gas or water vapour.

24. (canceled)

25. (canceled)

26. (canceled)

27. (canceled)