Method and apparatus for the measurement of the refractive index of a gas

Claim 2

An optical apparatus for measuring the absolute refractive index "n" of a gas, said apparatus comprising a light source and a vacuum cell optically aligned therewith and spatically separated therefrom, said cell comprising a pair of inner optically reflective surfaces separable by a distance "L" and means for varying said distance "L" varying the optical path length of light travel within said cell; first differential plane mirror interferometer means optically spaced between said light source and said vacuum cell and in optical alignment therewith, said first interferometer means having a first associated measurement leg optically disposed outside of said vacuum cell and in said gas to be measured; second differential plane mirror interferometer means optically spaced between said light source and said vacuum cell in optical alignment therewith, said second interferometer means having a second associated measurement leg optically disposed in said vacuum cell; first means optically connected to said first interferometer means for receiving an output therefrom for measuring a first phase variation in said first differential plane mirror interferometer means output for providing a first phase variation value as said distance "L" varies; second means optically connected to said said second interferometer means for receiving an output therefrom for providing a second phase variation value in said second differential plane mirror interferometer means output as said distance "L" varies; and means operatively connected to said first and second phase variation value providing means for receiving said first and second variation values and taking the ratio thereof for providing an output therefrom which is the absolute index of refraction "n" of said gas, said first and second differential plane mirror interferometer means being optically aligned with an input beam emitted from said light source, said first and second associated measurement legs having associated output beams, said pair of inner optically reflective surfaces being optically aligned with said associated output beams.

Claim 3

An apparatus in accordance with claim 1 wherein said cell further comprises a bellows having said pair of windows, said windows comprising transparent plano windows having diameters larger than the outside diameter of said bellows attached to each end of said bellows, one said pair of windows optically reflective surface comprising two high reflectivity mirror coating spots disposed for obtaining reflections from said one surface on the vacuum side of said transparent plano window and within the diameter of said bellows, the other of said pair of windows optically reflective surface comprising two high reflectivity mirror coating spots disposed for obtaining reflections from said other window reflective surface on the vacuum side of said other transparent plano window and outside the diameter of said bellows.

Claim 4

An apparatus in accordance with claim 2 wherein said distance varying means comprises means for varying said distance "L" between said highly reflective mirror coatings substantially between 0 and 100 millimeters.

Claim 5

An apparatus in accordance with claim 3 wherein said ratio taking means comprises a microcomputer.

Claim 6

An apparatus in accordance with claim 4 wherein said light source comprises a laser.

Claim 7

An apparatus in accordance with claim 5 wherein said emitted light comprises a beam having a pair of orthogonally polarized frequency components which are optically provided to said differential plane mirror interferometers for providing a plurality "N" of associated exit/return beams to said cell for each of said first and second differential plane mirror interferometer.

Claim 8

An apparatus in accordance with claim 6 wherein said first phase variation value providing means comprises first phase meter/accumulator means for providing a measured phase difference of M gas =NnL where n is the refractive index of gas and NL is the total physical length change through said gas experienced by said exit/return beams associated with said first differential plane mirror interferometer, said second phase variation value providing means providing a phase difference of M vac =NL as a known value, said ratio of said measured phase differences being M gas /M vac =NnL/NL=n for providing said refractive index n of said gas as said output as n=M gas /M vac .

Claim 9

An apparatus in accordance with claim 7 wherein N=4.

Claim 10

An apparatus in accordance with claim 6 wherein said first phase variation value providing means comprises first phase meter/accumulator means for providing a measured phase difference of M gas =NnL where n is the refractive index of the gas and NL is the total physical length change through said gas experienced by said exit/return beams associated with said first differential plane mirror interferometer, said second phase variation value providing means comprising second phase meter/accumulator means for providing a measured phase difference of M vac =NL where NL is the total physical length change through said vacuum experienced by said exit/return beams associated with said second differential plane mirror interferometer, said ratio of said measured phase differences being M gas /M vac =NnL/NL=n for providing said refractive index n of said gas as said output as n=M gas /M vac .

Claim 11

An apparatus in accordance with claim 9 wherein N=4.

Claim 12

An optical apparatus for measuring the absolute refractive index "n" of a gas, said apparatus comprising a light source and a vacuum cell optically aligned therewith and spatially separated therefrom, said cell comprising a pair of windows, said windows comprising a pair of inner optically reflective surfaces separable by a distance "L" and means for varying said distance "L" for varying the optical path length of light travel within said cell; first differential plane mirror interferometer means optically spaced between said light source and said vacuum cell and in optical alignment therewith, said first interferometer means having a first associate measurement leg optically disposed substantially equally in both said vacuum cell and outside of said vacuum cell in said gas to be measured; second differential plane mirror interferometer means optically spaced between said light source and said vacuum cell in optical alignment therewith, said second interferometer means having a second associated measurement leg optically disposed in said vacuum cell; means optically connected to said first interferometer means for receiving an output therefrom for measuring a first phase variation in said first differential plane mirror interferometer means output for providing a first phase variation value as said distance "L" varies; second means optically connected to said second interferometer means for receiving an output therefrom for providing a second phase variation value in said second differential plane mirror interferometer means output as said distance "L" varies; and means operatively connected to said first and second phase variation value providing means for receiving said first and second phase variation values and taking the ratio thereof for providing an output therefrom which is the absolute index of refraction of said gas minus one, represented by n-1, said first and second differential plane mirror interferometer means being optically aligned with an input beam emitted from said light source, said first and second associated measurement legs having associated output beams, said pair of inner optically reflective surfaces being optically aligned with said associated output beams.

Claim 13

An optical apparatus for measuring the absolute refractive index "n" of a gas, said apparatus comprising a light source and a vacuum cell optically aligned therewith and spatially separated therefrom, said cell comprising a pair of windows, said windows comprising a pair of inner optically reflective surfaces separable by a distance "L" and means for varying said distance "L" for varying the optical path length of light travel within said cell; first differential plane mirror interferometer means optically spaced between said light source and said vacuum cell and in optical alignment therewith, said first interferometer means having a first associate measurement leg optically disposed substantially equally in both said vacuum cell and outside of said vacuum cell in said gas to be measured; second differential plane mirror interferometer means optically spaced between said light source and said vacuum cell in optical alignment therewith, said second interferometer means having a second associated measurement leg optically disposed in said vacuum cell; means optically connected to said first interferometer means for receiving an output therefrom for measuring a first phase variation in said first differential plane mirror interferometer means output for providing a first phase variation value as said distance "L" varies; second means optically connected to said second interferometer means for receiving an output therefrom for providing a second phase variation value in said second differential plane mirror interferometer means output as said distance "L" varies; and means operatively connected to said first and second phase variation value providing means for receiving said first and second phase variation values and taking the ratio thereof for providing an output therefrom which is the absolute index of refraction of said gas minus one, represented by n-1, said first and second differential plane mirror interferometer means being optically aligned with an input beam emitted from said light source, said first and second associated measurement legs having associated output beams, said pair of inner optically reflective surfaces being optically aligned with said associated output beams.

Claim 14

An apparatus in accordance with claim 11 wherein said cell further comprises a bellows having said pair of windows, said windows comprising transparent plano windows having diameters larger than the outside diameter of said bellows attached to each end of said bellows, one of said pair of windows optically reflective surface comprising two high reflectivity mirror coating spots disposed for obtaining reflections from said one surface on the vacuum side of said transparent plano window and within the diameter of said bellows, the other of said pair of windows optically reflective surface comprising two high reflectivity mirror coating spots disposed for obtaining reflections from said other window reflective surface on the vacuum side of said other transparent plano window and outside the diameter of said bellows and two high reflectivity mirror coating spots disposed for obtaining reflections from said other window reflective surface on the vacuum side of said other transparent plano window and within the diameter of said bellows.

Claim 15

An apparatus in accordance with claim 12 wherein said distance varying means comprises means for varying said distance "L" between said highly reflective mirror coatings substantially between 0 and 100 millimeters.

Claim 16

An apparatus in accordance with claim 13 wherein said ratio taking means comprises a microcomputer.

Claim 17

An apparatus in accordance with claim 14 wherein said light source comprises a laser.

Claim 18

An apparatus in accordance with claim 15 wherein said emitted light comprises a beam having a pair of orthogonally polarized frequency components which are optically provided to said differential plane mirror interferometers for providing a plurality "N" of associated exit/return beams to said cell for each of said first and second differential plane mirror interferometer.

Claim 19

An apparatus in accordance with claim 16 wherein said first phase variation value providing means comprises first phase meter/accumulator means for providing a measured phase difference of M gas-vac =(n-1)NL where n is the refractive index of the gas and NL is the total physical length change through said gas experienced by said exit/return beams associated with said first differential plane mirror interferometer, said second phase variation value providing means comprising second phase meter/accumulator means for providing a measured phase difference of M vac =NL where NL is the total physical length change through said vacuum experienced by said exit/return beams associated with said second differential plane mirror interferometer, said ratio of said measured phase differences being M gas-vac /M vac =(n-1)NL/NL=n-1 for providing said refractive index n of said gas as said output as n=1+M gas-vac /M vac .

Claim 20

An apparatus in accordance with claim 17 wherein N=4.

Claim 21

An apparatus in accordance with claim 16 wherein said first phase variation value providing means comprises first phase meter/accumulator means for providing a measured phase difference of M gas-vac =(n-1)NL where n is the refractive index of the gas and NL is the total physical length change through said gas and vacuum experienced by said exit/return beams associated with said first differential plane mirror interferometer, said second phase variation value providing means providing a phase difference of M vac =NL as a known value, said ratio of said measured phase differences being M gas-vac /M vac =(n-1)NL/NL=n-1 for providing said refractive index n of said gas as said output as n=1+M gas-vac /M vac .

Claim 22

An apparatus in accordance with claim 19 wherein N=4.