Distributed Brillouin laser sensor
Brillouin fiber sensors can provide distributed measurements of parameters of interest over long distances in a fiber by measuring the Brillouin frequency shift as a function of position along the fiber. The Brillouin frequency shift may be determined, to within a small fraction of the Brillouin linewidth, by establishing a series of lasing modes that experience Brillouin amplification at discrete spatial locations in a test fiber. A linewidth narrowing and high intensity associated with the lasing transition enable precise measurements of the lasing frequency associated with each of the lasing modes. The Brillouin frequency may be determined based on the lasing frequency.
1. A system, comprising:
a lasing cavity comprising a fiber under test and a feedback fiber; and
a pulse pump generator transmitting a pump beam through the lasing cavity thereby generating stimulated Brillouin scattering traveling in a direction opposite to a direction of the pump beam, the pump beam exciting a plurality of lasing modes in the lasing cavity, the pump beam being pulsed at a repetition rate matching a round-trip time in the lasing cavity so that the stimulated Brillouin scattering amplifies plurality of lasing modes at discrete locations in the fiber under test.
2. The system of claim 1 , wherein each lasing mode of the plurality of lasing modes comprises a lasing frequency, the lasing frequency of the each lasing mode corresponding to a Brillouin resonance frequency at the discrete locations,
wherein the fiber under test comprises a parameter of interest,
wherein a change in the parameter of interest produces a Brillouin frequency shift at one of the discrete locations in the fiber under test,
wherein the system further comprises:
a lasing frequency determiner determining the lasing frequency; and
a processing unit cooperating with the lasing frequency determiner inferring the Brillouin resonance frequency in the fiber under test based on the lasing frequency and determining the change in the parameter of interest based on the Brillouin frequency shift.
3. The system of claim 1 , wherein the lasing frequency determiner comprises:
a photodetector cooperating with the lasing cavity; and
a local oscillator cooperating with the photodetector and the processing unit.
4. The system of claim 1 , further comprising:
an electro-optic modulator cooperating with the pulse pump generator and the lasing cavity, the electro-optic modulator being driven by the pump beam so as to mitigate mode competition.
5. The system of claim 1 , further comprising:
a polarization switch cooperating with the pulse pump generator so as to-mitigate polarization fading.
6. The system of claim 1 , wherein the lasing cavity comprises a ring cavity or a Fabry-Pérot laser cavity.
7. The system of claim 1 , wherein the feedback fiber is approximately equal to or longer than the fiber under test.
8. The system of claim 1 , wherein the fiber under test and the feedback fiber comprises single mode fiber.
9. A method, comprising:
providing a lasing cavity comprising a fiber under test and a feedback fiber; and
transmitting a pump beam through the lasing cavity using a pulse pump generator thereby generating stimulated Brillouin scattering traveling in a direction opposite to a direction of the pump beam, the pump beam exciting a plurality of lasing modes in the lasing cavity, the pump beam being pulsed at a repetition rate matching a round-trip time in the lasing cavity so that the stimulated Brillouin scattering amplifies plurality of lasing modes at discrete locations in the fiber under test.
10. The method of claim 9 , wherein the fiber under test comprises a parameter of interest,
wherein a change in the parameter of interest produces a Brillouin frequency shift at one of the discrete locations in the fiber under test,
wherein the method further comprises:
determining the in the parameter of interest based on the Brillouin frequency shift, using a processing unit.
11. The method of claim 10 , wherein each lasing mode of the plurality of lasing modes comprises a lasing frequency, the lasing frequency of each lasing mode corresponding to a Brillouin resonance frequency at the discrete locations,
wherein the method further comprises:
providing a lasing frequency determiner cooperating with the processing unit; and
inferring the Brillouin resonance frequency in the fiber under test based on the lasing frequency, using the processing unit and the lasing frequency determiner.
12. The method of claim 9 , further comprising:
mitigating mode competition with a pulse train with variable amplitude to adjust a round-trip loss experienced by each of the lasing modes, using an electro-optic modulator cooperating with the pulse pump generator and the lasing cavity.
13. The method of claim 9 , further comprising:
mitigating polarization fading with sequential pump sequences with orthogonal polarizations, using a polarization switch cooperating with the pulse pump generator.
14. The method of claim 9 , wherein the lasing cavity comprises at least one of a ring cavity or a Fabry-Pérot laser cavity.
15. The method of claim 14 , wherein the ring cavity comprises the fiber under test and the feedback fiber that is approximately equal to or longer than the fiber under test.
16. The method of claim 9 , wherein the fiber under test and the feedback fiber comprises single mode fiber.