Apparatus and method for precision adjustment of interferometer pathlength difference

Claim 3

The method of claim 1 wherein the step of adjusting the length of one of the arms includes the step of reducing the length of one of the arms to produce a null signal output from the interferometer.

Claim 4

The method of claim 2, further including the step of adjusting the arms to propagate substantially equal light intensities.

Claim 5

The method of claim 2, further including the steps of: forming the interferometer such that the first arm comprises a first optical fiber and the second arm comprises a second optical fiber; determining the refractive index of a selected one of the optical fibers; and removing a length of fiber from the selected fiber to produce a null signal output from the interferometer.

Claim 6

The method of claim 4, further including the step of adjusting the arms to propagate substantially equal light intensities.

Claim 7

The method of claim 4, further including the steps of: modulating the intensity of the incoherent light at a predetermined modulation frequency; and producing the null signal at a predetermined multiple of a fundamental frequency of the interferometer.

Claim 8

The method of claim 6 wherein the step of measuring the refractive index includes the step of measuring the null signal for a known length of the selected fiber and calculating the refractive index using the equation n=mc/(2Lf m ) where n is the refractive index of the fiber, c is the free space velocity of light, m is an odd integer, L is the length of the fiber, and f m is the null frequency corresponding to the m th multiple of the fundamental frequency.

Claim 9

The method of claim 6, further including the steps of: (a) forming the interferometer such that the first arm comprises a first optical fiber and the second arm comprises a second optical fiber, the optical fibers providing an optical pathlength difference ΔL o ; (b) determining the refractive index of a selected one of the optical fibers; and (c) measuring the null frequency with an initial predetermined frequency resolution bandwidth; (d) calculating an initial length resolution using the equation ΔL=mcΔf/(2nf m 2 ), where n is the refractive index of the fiber, c is the free space velocity of light, m is an odd integer, and f m is the null frequency corresponding to the m th multiple of fundamental frequency of the interferometer; (e) reducing the length of the selected fiber; (f) reducing the frequency resolution bandwidth to a new predetermined value; (g) measuring the null frequency at the new frequency resolution bandwidth; and (h) repeating steps (d) through (g) until a predetermined length resolution is obtained.

Claim 10

The method of claim 8 further including the step of adjusting the arms to propagate substantially equal light intensities.

Claim 11

The method of claim 3, further including the steps of: (a) setting the lengths of the arms to have an initial optical pathlength difference L o ; (b) determining a frequency corresponding to a null signal output from the interferometer; (c) calculating the refractive index using the equation n=mc/(2f m L o ) where n is refractive index, c is the free space velocity of light, m is an integer, and f m is the null frequency corresponding to the m th multiple of a fundamental frequency for th interferometer; (d) removing a length x of fiber from the selected arm so that the pathlength difference is L o -x; (e) measuring the m th null frequency corresponding to the pathlength difference L o -x; (f) calculating x using the equation f -1 =(2nL o /c)+(2nx/c); and (g) repeating steps (c) through (f) until a predetermined pathlength difference is obtained.

Claim 12

The method of claim 1, further including the steps of: (a) forming the interferometer such that the first arm comprises a first optical fiber and the second arm comprises a second optical fiber, the optical fibers providing an optical pathlength difference ΔL o ; (b) determining the refractive index of a selected one of the optical fibers; and (c) measuring the null frequency with an initial predetermined frequency resolution bandwidth; (d) calculating an initial length resolution using the equation ΔL=mcΔf/(2nf m 2 ), where n is the refractive index of the fiber, c is the free space velocity of light, m is an odd integer, and f m is the null frequency corresponding to the m th multiple of fundamental frequency of the interferometer; (e) reducing the length of the selected fiber; (f) reducing the frequency resolution bandwidth to a new predetermined value; (g) measuring the null frequency at the new frequency resolution bandwidth to determined a new length resolution; and (h) repeating steps (d) through (f) until a predetermined length resolution is obtained.

Claim 13

The method of claim 11, further including the step of adjusting the arms to propagate substantially equal light intensities.

Claim 14

Apparatus for adjusting the pathlength difference in a pathlength mismatched interferometer having a first arm and a second arm, comprising: means for inputting portions of intensity modulated incoherent light into the first and second arms; means for monitoring signals output from the interferometer; and means for adjusting the length of one of the arms to produce a predetermined signal output from the interferometer.

Claim 15

Apparatus for adjusting the pathlength difference in a pathlength mismatched interferometer having a first arm and a second arm, comprising: means for inputting portions of intensity modulated incoherent light into the first and second arms; means for monitoring signals output from the interferometer; and means for adjusting the length of one of the arms to produce a predetermined signal output from the interferometer.

Claim 16

The apparatus of claim 13 wherein the means for adjusting the length of one of the arms includes means for reducing the length of one of the arms to produce a null signal output from the interferometer.

Claim 17

The apparatus of claim 14, further including means for adjusting the arms to propagate substantially equal light intensities.

Claim 18

The apparatus of claim 15, further including: means for forming the interferometer such that the first arm comprises a first optical fiber and the second arm comprises a second optical fiber; means for determining the refractive index of a selected one of the optical fibers; and means for removing a length of fiber from the selected fiber to produce a null signal output from the interferometer.

Claim 19

The apparatus of claim 16, further including means for adjusting the arms to propagate substantially equal light intensities.

Claim 20

The apparatus of claim 16, further including: means for modulating the intensity of the incoherent light at a predetermined modulation frequency; and means for producing the null signal at a predetermined multiple of the modulation frequency.

Claim 21

The apparatus of claim 18 wherein the means for measuring the refractive index includes: means for measuring the null signal for a known length of the selected fiber; and computing means for calculating the refractive index using the equation n=mc/(2Lf m ) where n is the refractive index of the fiber, c is the free space velocity of light, m is an odd integer, L is the length of the fiber, and f m is the null frequency corresponding to the integer m.

Claim 22

The apparatus of claim 13, wherein the interferometer is formed such that the first arm comprises a first optical fiber and the second arm comprises a second optical fiber, further including: means for determining the refractive index of a selected one of the optical fibers; means for measuring the null frequency with an initial predetermined frequency resolution bandwidth to determine an initial length resolution; means for reducing the length of the selected fiber; means for reducing the frequency resolution bandwidth to a new predetermined value; means for measuring the null frequency at the new frequency resolution bandwidth to determine a new length resolution.

Claim 23

The apparatus of claim 14, wherein the interferometer is formed such that the first arm comprises a first optical fiber and the second arm comprises a second optical fiber, further including: means for determining the refractive index of a selected one of the optical fibers; means for measuring the null frequency with an initial predetermined frequency resolution bandwidth to determine an initial length resolution; means for reducing the length of the selected fiber; means for reducing the frequency resolution bandwidth to a new predetermined value; and means for measuring the null frequency at the new frequency resolution bandwidth to determine a new length resolution.