System and method for monitoring environmental effects using optical sensors

• US 7,119,325 B2
• Filed: 01/27/2004
• Issued: 10/10/2006
• Est. Priority Date: 01/27/2003
• Status: Expired due to Fees

• Current Assignee: Newport Corporation (MKS Instruments Incorporated)
• Original Assignee: Bookham Incorporated (Oclaro (North America), Inc.)
• Inventors: Nguyen, Hoang, Pieterse, Jan-Willem, Cordes, Andrew H., Abriam, Rosemary O.
• Primary Examiner(s): Allen, Stephone B.
• Application Number:
  US10/766,306
• Publication Number:
  US 20040245441A1
• Time in Patent Office: 987 Days
• Field of Search: 25022714-22718, 356/73.1, 356477-482, 385/12
• US Class Current: 250/227.14
• CPC Class Codes: G01D 5/35303 using a reference fibre, e.g. interferometric devices
• CPC Class Codes: G01D 5/35316 using a Bragg gratings
• CPC Class Codes: G01D 5/35354 Sensor working in reflection
• CPC Class Codes: G01J 3/1895 using fiber Bragg gratings or gratings integrated in a waveguide
• CPC Class Codes: G01J 3/28 Investigating the spectrum using colour filters G01J3/51
• CPC Class Codes: G01J 3/433 Modulation spectrometry; Derivative spectrometry

Abstract

An apparatus and method for determining a physical parameter affecting an optical sensor or a number of sensors in a network. The apparatus uses a narrow linewidth source at an emission wavelength λ_e and an arrangement for varying the emission wavelength λ_e of the radiation. An analysis module with curve fitting is used to generate a fit to the response signal obtained from the optical sensor. The physical parameter is determined form the fit rather than from the response signal. The apparatus can be employed with Bragg gratings, etalons, Fabry Perot elements or other optical sensors.

Claims

1. An apparatus for use with an optical sensor, said apparatus comprising:

a source emitting radiation at an emission wavelength;

a wavelength meter coupled to monitor said emission wavelength;

means for varying said emission wavelength coupled to said wavelength meter;

an optical path guiding said radiation to said optical sensor and guiding a response radiation from said optical sensor;

a detector generating a response signal to said response radiation; and

an analysis module which analyzes said response signal and determines therefrom a physical parameter by;

detecting peaks in said response signal by applying a threshold level;

identifying a full width half maximum of each peak;

identifying a centroid of each peak from one full width half maximum; and

making a fit to each peak.

2. The apparatus of claim 1, wherein said source is a laser.

3. The apparatus of claim 2, wherein said laser is selected from the group consisting of External Cavity Diode lasers, Distributed Bragg Reflector lasers, and fiber lasers.

4. The apparatus of claim 1, wherein said fit is a best fit curve.

5. The apparatus of claim 1, wherein said optical sensor is selected from the group consisting of Bragg Grating and Fabry-Perot elements.

6. The apparatus of claim 5, wherein said optical path comprises an optical fiber and said Bragg Grating is a Fiber Bragg Grating.

7. The apparatus of claim 1, wherein said means for varying said emission wavelength comprises a laser tuner.

8. The apparatus of claim 7, wherein said laser tuner comprises a scanner for scanning said emission wavelength.

9. The apparatus of claim 7, wherein said laser tuner comprises a sweeper for sweeping said emission wavelength.

10. The apparatus of claim 1, wherein said optical path comprises a waveguide.

11. The apparatus of claim 1, further comprising a tap for tapping said radiation and coupling said radiation to said wavelength meter for monitoring said emission wavelength.

12. A method for determining a physical parameter affecting an optical sensor, said method comprising:

emitting a radiation having an emission wavelength;

providing an optical path for said radiation to said optical sensor and for a response radiation from said optical sensor;

varying said emission wavelength;

generating a response signal from said response radiation; and

determining said physical parameter by;

detecting peaks in said response signal by applying a threshold level;

identifying a full width half maximum of each peak;

identifying a centroid of each peak from the full width half maximum; and

making a fit to each peak.

13. The method of claim 12, wherein said optical sensor produces said response radiation by a varying a property of said radiation, said property being selected from the group consisting of transmittance, reflectance, absorbance and polarization.

14. The method of claim 12, wherein said emission wavelength is varied continuously.

15. The method of claim 14, wherein said emission wavelength is swept.

16. The method of claim 12, wherein said emission wavelength is varied discontinuously.

17. The method of claim 16, wherein said emission wavelength is scanned.

18. The method of claim 12, wherein said making a fit comprises making a fit selected from the group consisting of a polynomial fit, a Lorentzian fit and a Gaussian fit.

19. The method of claim 12, wherein said physical parameter is selected from the group consisting of temperature, strain and pressure.

20. The method of claim 12, further comprising tapping said radiation and monitoring said emission wavelength.