Apparatus and method for reducing phase errors in an interferometer

• US 5,153,676 A
• Filed: 08/21/1991
• Issued: 10/06/1992
• Est. Priority Date: 04/26/1983
• Status: Expired due to Term

• Current Assignee: Board of Trustees of the Leland Stanford Junior University (Stanford Management Co.)
• Original Assignee: Board of Trustees of the Leland Stanford Junior University (Stanford Management Co.)
• Inventors: Bergh, Ralph A.
• Primary Examiner(s): Turner, Samuel A.
• Application Number:
  US07/747,989
• Time in Patent Office: 412 Days
• Field of Search: 356/350
• US Class Current: 356/460
• CPC Class Codes: G01C 19/721 Details

Abstract

A fiber optic rotation sensor comprises a fiber optic interferometer loop formed from a highly birefringent optical fiber, and a short coherence length source for introducing light into the inteferometer loop to provide a pair of waves which counter-propogate therethrough. A detector is included to detect the phase difference between the waves after they have traversed the loop to provide an indication of the loop rotation rate, in accordance with the Sagnac effect. Phase errors are reduced by selecting the coherence length of the source and the birefringence of the fiber, so that the loop is comprised of plural fiber coherence lengths. The term "fiber coherence length" should be distinguished from source coherence length. Fiber coherence length is the length of fiber required for the optical path length difference between the two polarization modes of a single mode fiber to equal one coherence length of the light source. In addition, phase errors are reduced by providing a birefringent waveguide between the source and the loop such that light propagates from the source to the loop in an optical path having a path length difference which is at least equal to a coherence length of the source. Phase errors are further reduced by positioning the detector to intercept the optical output signal from the loop such that light wave components in orthogonal modes are spatially averaged.

Claims

1. An interferometer which provides an optical output signal, said interferometer comprising:

an interferometer loop comprised of birefringent waveguide which propagates light in first and second orthogonal polarization modes, the birefringence of said waveguide causing light in said first and second modes to propagate around said loop in first and second propagation times, respectively corresponding to first and second optical path lengths, respectively, said first optical path length being different from said second optical path length to provide an optical path length difference therebetween;

a light source providing light for input to said loop, said light having a coherence length which is at least about a hundred times less than the optical path length difference for said first and second modes to reduce phase errors caused by non-orthogonal components of said output signal;

an optical propagation path between said light source and said loop, said optical propagation path comprised of birefringent waveguide which propagates light in two polarization modes, the birefringence of said waveguide causing light in said two orthogonal polarization modes to propagate from said source to said loop in third and fourth propagation times corresponding to third and fourth optical path lengths, respectively, said third and fourth optical path lengths having an optical path length difference therebetween which is equal to at least one coherence length of the source to reduce phase errors caused by non-orthogonal components of said output signal;

a first coupler for coupling light between said optical propagation path and said loop, said coupler comprised of two waveguides each having two axes of birefringence, one of said axes being a fast axis and the other being a slow axis, said axes being aligned to couple light from one fast axes to another fast axis and from one slow axis to another slow axes without substantial coupling between a fast axis and a slow axis, said coupler coupling light from said loop to said optical propagation path to form said optical output signal;

a detector; and

a second coupler for coupling said optical output signal from said optical propagation path to said detector, said optical output signal propagating in two orthogonal polarization modes, said detector sized and positioned to intercept the optical output signal so as to detect light from both of the orthogonal polarization modes, such that light wave components in orthogonal modes of said optical output signal are spatially averaged so as to reduce phase errors resulting from orthogonal components of said signal.

2. The interferometer of claim 1, wherein said optical propagation path is comprised of a birefringent optical fiber.

3. The interferometer of claim 1, wherein said first coupler is comprised of juxtaposed optical fibers.

4. The interferometer of claim 1, wherein said second coupler is comprised of juxtaposed optical fibers.

5. The interferometer of claim 1, wherein said light in said optical propagation path is of substantially equal intensity for each of said two polarization modes of said optical propagation path.

6. The interferometer of claim 1, wherein the scattering rate from one polarization mode to the other in said interferometer loop is less than 1% per kilometer.

7. The interferometer of claim 1, wherein the coherence length is at least several hundred times less than the optical path length difference for the modes of said interferometer loop.

8. The interferometer of claim 1, wherein the light in said interferometer loop is of substantially equal intensity for each of the polarization modes of the interferometer loop.

9. The interferometer of claim 1, wherein said orthogonal light wave components are spatially averaged under conditions of global orthogonality.

10. A method of reducing phase errors in an interferometer having an interferometer loop comprised of single mode birefringent waveguide which propagates light in two orthogonal polarization modes, said interferometer providing an output signal having both orthogonal and non-orthogonal light wave components, said method comprising:

utilizing a light source having a coherence length which is at least about a hundred times less than the optical path length difference around said loop for said two modes to reduce phase errors caused by interference between non-orthogonal light wave components of said signal;

propagating light from said source through birefringent waveguide disposed between the source and the loop such that, upon entering said loop, light in one polarization mode is substantially incoherent with respect to light in the other polarization mode to reduce phase errors caused by interference between non-orthogonal light wave components of said signal; and

spatially averaging orthogonal light wave components of said signal under conditions of global orthogonality to reduce phase errors resulting from orthogonal light wave components of said signal.

11. An interferometer which provides an optical output signal, said interferometer comprising:

an interferometer loop comprised of birefringent waveguide which propagates light in first and second orthogonal polarization modes, the birefringence of said waveguide causing light in said first and second modes to propagate around said loop in first and second propagation times, respectively corresponding to first and second optical path lengths, respectively, said first optical path length being different from said second optical path length to provide an optical path length difference therebetween;

a light source providing light for input to said loop, said light having a coherence length which is at least about a hundred times less than the optical path length difference for said first and second modes to reduce phase errors caused by non-orthogonal components of said output signal;

an optical propagation path between said light source and said loop, said optical propagation path comprised of birefringent waveguide which propagates light in two polarization modes, the birefringence of said waveguide causing light in said two orthogonal polarization modes to propagate from said source to said loop in third and fourth propagation times corresponding to third and fourth optical path lengths, respectively, said third and fourth optical path lengths having an optical path length difference therebetween which is equal to at least one coherence length of the source to reduce phase errors caused by non-orthogonal components of said output signal;

a first coupler for coupling light between said optical propagation path and said loop, said coupler coupling light from said loop to said optical propagation path to form said optical output signal, said optical output signal propagating in said optical propagation path in two orthogonal polarization modes; and

a detector sized and positioned to intercept the optical output signal so as to detect light from both of the orthogonal polarization modes, such that light wave components in orthogonal modes of said optical output signal are spatially averaged so as to reduce phase errors resulting from orthogonal components of said signal.

12. The interferometer of claim 11, wherein said optical propagation path is comprised of a birefringent optical fiber.

13. The interferometer of claim 11, wherein said coupler is comprised of juxtaposed optical fibers.

14. The interferometer of claim 11, additionally comprising a second coupler for coupling said optical output signal from said optical propagation path to said detector.

15. The interferometer of claim 11, wherein light in said optical propagation path is of substantially equal intensity for each of two polarization modes of said optical propagation path.

16. The interferometer of claim 11, wherein the scattering rate from one polarization mode to the other in said interferometer loop is less than 1% per kilometer.

17. The interferometer of claim 11, wherein the coherence length is at least several hundred times less than the optical path length difference for the modes of said interferometer loop.

18. The interferometer of claim 11, wherein light in said interferometer loop is of substantially equal intensity for each of two polarization modes of the interferometer loop.

19. The interferometer of claim 11, wherein said orthogonal light wave components are spatially averaged under conditions of global orthogonality.