IP Library Granted Patent US 9,025,157
Granted Patent B2
US 9,025,157 · App. 13/745,663 · Granted May 5, 2015

System and method for measuring perturbations using a slow-light fiber Bragg grating sensor

Inventors: He Wen (Menlo Park, CA); Michel J. F. Digonnet (Palo Alto, CA); Shanhui Fan (Stanford, CA)
Assignee: The Board of Trustees of the Leland Stanford Junior University
G01J1/0407G01D5/35316G01K11/3206G01L1/246G02B6/02204G02B6/29353
View Patent ↗
Loading inventors, assignments & file history…
Monitor This Case
Get email alerts when status or documents change.
Order Certified Copies
Most orders are placed with the USPTO same day — all within 24 business hours.
Order via The Patent Place →
Pre-filled with this patent's details
Quick Facts
Patent No.
US 9,025,157
App. No.
13/745,663
Granted
May 5, 2015
Kind
B2
Abstract

An optical device, a method of configuring an optical device, and a method of using a fiber Bragg grating is provided. The optical device includes a fiber Bragg grating, a narrowband optical source, and at least one optical detector. The fiber Bragg grating has a power transmission spectrum as a function of wavelength with one or more resonance peaks, each comprising a local maximum and two non-zero-slope regions with the local maximum therebetween. The light generated by the narrowband optical source has a wavelength at a non-zero-slope region of a resonance peak that is selected such that one or more of the following quantities, evaluated at the resonance peak, is at a maximum value: (a) the product of the group delay spectrum and the power transmission spectrum and (b) the product of the group delay spectrum and one minus the power reflection spectrum.

Claims (32)

1. An optical device comprising:

a fiber Bragg grating comprising a substantially periodic refractive index modulation along a length of the fiber Bragg grating, wherein the fiber Bragg grating has a power reflection spectrum as a function of wavelength, a power transmission spectrum as a function of wavelength, and a group delay spectrum as a function of wavelength;

a narrowband optical source in optical communication with the fiber Bragg grating and configured to transmit light to the fiber Bragg grating such that a transmitted portion of the light is transmitted along the length of the fiber Bragg grating and a reflected portion of the light is reflected from the fiber Bragg grating, wherein the power transmission spectrum as a function of wavelength comprises one or more resonance peaks, each comprising a local maximum and two non-zero-slope regions with the local maximum therebetween; and

at least one optical detector configured to detect an optical power of the transmitted portion of the light, the reflected portion of the light, or both the transmitted portion of the light and the reflected portion of the light,

wherein the light has a wavelength at a non-zero-slope region of a resonance peak of the one or more resonance peaks, wherein the resonance peak is selected such that one or more of the following quantities, evaluated at the resonance peak, is at a maximum value: (a) the product of the group delay spectrum and the power transmission spectrum and (b) the product of the group delay spectrum and one minus the power reflection spectrum.

2. The optical device of claim 1 , wherein the product of the group delay spectrum and the power transmission spectrum, evaluated at the resonance peak, is at a maximum value, and the at least one optical detector is configured to detect the optical power of the transmitted portion of the light.

3. The optical device of claim 1 , wherein the product of the group delay spectrum and one minus the power reflection spectrum, evaluated at the resonance peak, is at a maximum value and the at least one optical detector is configured to detect the optical power of the reflected portion of the light.

4. The optical device of claim 1 , wherein the detected optical power is indicative of an amount of strain applied to the fiber Bragg grating.

5. The optical device of claim 1 , wherein the detected optical power is indicative of a temperature of the fiber Bragg grating.

6. The optical device of claim 1 , wherein the detected optical power is indicative of a magnitude of a magnetic field or an electric field applied to the fiber Bragg grating.

7. The optical device of claim 1 , further comprising a feedback control system configured to stabilize the optical device against thermal fluctuations.

8. A method of using a fiber Bragg grating comprising:

providing a fiber Bragg grating comprising a substantially periodic refractive index modulation along a length of the fiber Bragg grating, wherein the fiber Bragg grating has a power reflection spectrum as a function of wavelength, a power transmission spectrum as a function of wavelength, and a group delay spectrum as a function of wavelength, wherein the power transmission spectrum as a function of wavelength comprises one or more resonance peaks, each comprising a local maximum and two non-zero-slope regions with the local maximum therebetween;

generating light from a narrowband optical source, the narrowband optical source in optical communication with the fiber Bragg grating such that a transmitted portion of the light is transmitted along the length of the fiber Bragg grating and a reflected portion of the light is reflected from the fiber Bragg grating; and

detecting an optical power of the transmitted portion of the light, the reflected portion of the light, or both the transmitted portion of the light and the reflected portion of the light with at least one optical detector,

wherein the light has a wavelength at a non-zero-slope region of a resonance peak of the one or more resonance peaks, wherein the resonance peak is selected such that one or more of the following quantities, evaluated at the local maximum of the resonance peak, is at a maximum value: (a) the product of the group delay spectrum and the power transmission spectrum, and (b) the product of the group delay spectrum and one minus the power reflection spectrum.

9. The method of claim 8 , wherein the product of the group delay spectrum and the power transmission spectrum, evaluated at the local maximum of the resonance peak, is at a maximum value and detecting the optical power comprises detecting the optical power of the transmitted portion of the light.

10. The method of claim 8 , wherein the product of the group delay spectrum and one minus the power reflection spectrum, evaluated at the local maximum of the resonance peak, is at a maximum value and detecting the optical power comprises detecting the optical power of the reflected portion of the light.

11. The method of claim 8 , wherein the detected optical power is indicative of an amount of strain applied to the fiber Bragg grating.

12. The method of claim 8 , wherein the detected optical power is indicative of a temperature of the fiber Bragg grating.

13. The method of claim 8 , wherein the detected optical power is indicative of a magnitude of a magnetic field or an electric field applied to the fiber Bragg grating.

14. The method of claim 8 , wherein the substantially periodic refractive index modulation has an amplitude which varies along the length of the fiber Bragg grating such that the fiber Bragg grating is an apodized grating.

15. A method of configuring an optical device to be used as an optical sensor, the optical device comprising a fiber Bragg grating and a narrowband optical source in optical communication with the fiber Bragg grating, the narrowband optical source configured to transmit light to the fiber Bragg grating such that a transmitted portion of the light is transmitted along the length of the fiber Bragg grating and a reflected portion of the light is reflected from the fiber Bragg grating, the fiber Bragg grating comprising a substantially periodic refractive index modulation along a length of the fiber Bragg grating, the method comprising:

determining at least one of a power reflection spectrum of the light as a function of wavelength for the fiber Bragg grating and a power transmission spectrum of the light as a function of wavelength for the fiber Bragg grating, wherein the power transmission spectrum as a function of wavelength comprises one or more resonance peaks, each comprising a local maximum and two non-zero-slope regions with the local maximum therebetween;

determining a group delay spectrum of the light as a function of wavelength for the fiber Bragg grating;

selecting a resonance peak of the one or more resonance peaks, the resonance peak selected such that one or more of the following quantities, evaluated at the local maximum of the selected resonance peak, is at a maximum value: (a) a product of the group delay spectrum and the power transmission spectrum and (b) a product of the group delay spectrum and one minus the power reflection spectrum; and

configuring the fiber Bragg grating and the narrowband optical source such that the light from the narrowband light source has a wavelength at a non-zero-slope region of the two non-zero-slope regions of the selected resonance peak.

16. The method of claim 15 , wherein the optical device further comprises at least one optical detector configured to detect an optical power of the transmitted portion of the light, the reflected portion of the light, or both the transmitted portion of the light and the reflected portion of the light.

17. The method of claim 16 , wherein the product of the group delay spectrum and the power transmission spectrum, evaluated at the local maximum of the selected resonance peak, is at a maximum value and the at least one optical detector is configured to detect the optical power of the transmitted portion of the light.

18. The method of claim 16 , wherein the product of the group delay spectrum and one minus the power reflection spectrum, evaluated at the local maximum of the selected resonance peak, is at a maximum value and the at least one optical detector is configured to detect the optical power of the reflected portion of the light.

19. The method of claim 16 , wherein configuring the fiber Bragg grating and the narrowband optical source comprises tuning the narrowband light source to generate light having the wavelength at the non-zero-slope region of the two non-zero-slope regions of the selected resonance peak.

20. The method of claim 16 , wherein configuring the fiber Bragg grating and the narrowband optical source comprises selecting the fiber Bragg grating such that the wavelength is at the non-zero-slope region of the two non-zero-slope regions of the selected resonance peak.

Assignments (1)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Apr 17, 2013
From: WEN, HE; DIGONNET, MICHEL J.F.; FAN, SHANHUI
To: BOARD OF TRUSTEES OF THE LELAND STANFORD JUNIOR UNIVERSITY, THE
Reel/Frame 030231/0760 →
Continuity (4)
Continuation In Part 13224985 · Sep 2, 2011
Provisional Application 61589248 · Jan 20, 2012
Provisional Application 61381032 · Sep 8, 2010
Related Publication 20130193961A1 · Aug 1, 2013