System for multiplexed high resolution measurement of frequency variations in multimode fiber laser acoustic sensors

• US 5,867,258 A
• Filed: 10/27/1997
• Issued: 02/02/1999
• Est. Priority Date: 07/31/1997
• Status: Expired due to Term

• Current Assignee: Northrop Grumman Systems Corporation (Northrop Grumman Corporation)
• Original Assignee: Litton Systems Incorporated
• Inventors: Bell, Steven G., Frederick, Donald A.
• Primary Examiner(s): Turner, Samuel A.
• Application Number:
  US08/958,365
• Time in Patent Office: 463 Days
• Field of Search: 356/345, 356/352, 356/35.5, 250/227.14, 250/227.19, 250/227.27, 385/12, 385/14, 372/6
• US Class Current: 356/35.5
• CPC Class Codes: G01H 9/004 using fibre optic sensors light guides per se G02B6/00, acousto-optical devices specially adapted for gating or modulating in optical wave guides G02F1/125

Abstract

A system for performing high resolution measurement of frequency variations in multimode fiber laser acoustic sensors having an end-pumped active fiber sensor emitting a plurality of lasing modes, wherein precise frequencies of the lasing modes emitted are dependent upon a strain acting on said acoustic sensor. An optical fiber is connected to the active fiber sensor for transmitting the lasing modes. The optical fiber transmits the multiple lasing modes to an optical amplifier fiber where the lasing mode signals are amplified. The amplified lasing modes signals are then fed through a phase modulator connected to the optical fiber for applying a phase generated carrier on the lasing mode signals. The output from the phase modulator is supplied to a receiving interferometer having a predetermined path imbalance for interferometrically analyzing the frequency shifts of each of the lasing mode signals, wherein the predetermined path imbalance is matched with the longitudinal mode spacing between the lasing modes of the active fiber sensor. A demodulation unit is connected to the receiving interferometer for receiving and demodulating the output of the receiving interferometer to determine the frequency shift incurred by the lasing mode signals, wherein the demodulated frequency shift is proportional to the strain acting on the acoustic sensor. In an alternative embodiment, a plurality of active fiber sensors may be pumped by a single laser light source with their outputs multiplexed together and fed through the receiving interferometer for interferometric analysis of all the signals.

Claims

1. A system for performing high resolution measurement of frequency variations in multimode fiber laser acoustic sensors, comprising:

an end-pumped fiber laser emitting a plurality of lasing modes, wherein the frequencies of said lasing modes emitted are determined by the strain acting on said laser;

an optical fiber connected to said fiber laser for transmitting said lasing modes;

an amplifier means connected to said optical fiber for amplifying said lasing modes;

a phase modulator connected to said optical fiber for phase modulating a carrier on said lasing modes;

a receiving interferometer having a given path imbalance connected to said phase modulator through said optical fiber for generating interference fringes between portions of said lasing modes, wherein said portions have phase delays with respect to one another; and

sensing means connected to said receiving interferometer through said optical fiber for demodulating the fringe phase of said interference fringes, wherein said demodulated fringe phase is proportional to the strain acting on said fiber laser.

2. The system for performing high resolution measurement of frequency variations in multimode fiber laser acoustic sensors of claim 1, wherein said receiving interferometer is a pressure insensitive interferometer and said path imbalance is matched with an integral multiple of a round-trip cavity length of said laser fiber so that each of said phase shifts between fringe patterns of different lasing modes are an integral multiple of 2π

from one another and all said phase shifts for said lasing modes are in phase with one another.

3. The system for performing high resolution measurement of frequency variations in multimode fiber laser acoustic sensors of claim 2, wherein a signal-to-noise ratio of the output of said receiving interferometer for all of said plurality of lasing modes is similar to a signal-to-noise ratio achieved by interrogating said receiving interferometer with a single mode.

4. The system for performing high resolution measurement of frequency variations in multimode fiber laser acoustic sensors of claim 1, wherein said end-pumped fiber laser includes an erbium-doped optical fiber situated between two Bragg gratings.

5. The system for performing high resolution measurement of frequency variations in multimode fiber laser acoustic sensors of claim 1, further comprising:

at least one additional fiber laser emitting a plurality of lasing modes; and

a plurality of Bragg gratings connected between said receiving interferometer and said sensing means, wherein each of said Bragg gratings allows only a signal of a given wavelength associated with a respective fiber laser to be transmitted to said sensing means.

6. The system for performing high resolution measurement of frequency variations in multimode fiber laser acoustic sensors of claim 5, wherein each of said Bragg gratings is frequency matched with a respective fiber laser.

7. The system for performing high resolution measurement of frequency variations in multimode fiber laser acoustic sensors of claim 1, further comprising:

at least one additional fiber laser emitting a plurality of lasing modes with an optical fiber connected thereto for transmitting said lasing modes; and

a phase modulator respectively connected to each additional optical fiber for phase modulating a carrier frequency on said lasing modes;

wherein said carrier frequency phase modulated on lasing modes on each optical fiber is different from the carrier frequency phase modulated on all other optical fibers.

8. The system for performing high resolution measurement of frequency variations in multimode fiber laser acoustic sensors of claim 7, further comprising an optical coupler for coupling each of said optical fibers together so that all of said phase modulated lasing modes from all of said fiber lasers are transmitted along a single output lead, wherein said single output lead is fed into said receiving interferometer.

9. The system for performing high resolution measurement of frequency variations in multimode fiber laser acoustic sensors of claim 8, wherein said sensing means is able to electronically discriminate between the different fiber lasers based upon their respective carrier frequency.

10. The system for performing high resolution measurement of frequency variations in multimode fiber laser acoustic sensors of claim 7, wherein each optical fiber includes at least one additional fiber laser lasing at a different wavelength, so that each optical fiber carries a plurality of wavelengths at a unique carrier frequency.

11. The system for performing high resolution measurement of frequency variations in multimode fiber laser acoustic sensors of claim 10, further comprising:

a second optical coupler positioned between said receiving interferometer and said sensing means for branching off the output of said receiving interferometer onto a plurality of output leads; and

a plurality of Bragg gratings connected between said output leads and said sensing means, wherein each output lead has a Bragg grating respectively connected thereto for branching off a distinct lasing wavelength to be transmitted to said sensing means,

wherein said sensing means is able to electronically discriminate between the different fiber lasers based upon their respective carrier frequency.