Method for measuring the parameters of optical fibers

Claim 1

A method of measuring the diameter, D C , of the core of a clad optical fiber, given the thickness of the cladding layer, t, and the refractive indices of the cladding and core, m 1 and m 2 , respectively, which comprises: directing a beam of spatially coherent, monochromatic radiation at said fiber thereby to generate a complex scattering pattern, at least a portion of said pattern including contributions from the diffraction, the reflection and the refraction of said beam by said fiber, said scattering pattern being spatially radially disposed about said fiber and having a fringe pattern intensity modulation superimposed thereon; at a given reference angle θ R , measuring the modulation pattern over a scattering angle range Δθ R , where θ R satisfies the relationship: θ.sub.R × 1/2Δθ.sub.R < θ.sub.F and θ F is the cut-off angle which satisfies the relation: m.sub.1 cos (θ.sub.F /2) = 1; determining the core-to-fiber diameter ratio, R, by comparing said measured modulation pattern with modulation patterns priorly observed for clad optical fibers of the same core and cladding indices, measured at the same scattering angle range Δθ R ; and then computing said core diameter D C from the equation: D.sub.C = 2Rt/(1 - R).

Claim 2

A method of measuring the diameter, D C , of the core of a clad optical fiber, given the thickness of the cladding layer, t, and the refractive indices of the cladding and core, m 1 and m 2 , respectively, which comprises: directing a beam of spatially coherent, monochromatic radiation at said fiber thereby to generate a complex scattering pattern, at least a portion of said pattern including contributions from the diffraction, the reflection and the refraction of said beam by said fiber, said scattering pattern being spatially radially disposed about said fiber and having a fringe pattern intensity modulation superimposed thereon; at a given reference angle θ R , measuring the modulation pattern over a scattering angle range Δθ R , where θ R satisfies the relationship: θ.sub.R × 1/2Δθ.sub.R < θ.sub.F and θ F is the cut-off angle which satisfies the relation: m.sub.1 cos (θ.sub.F /2) = 1; determining the core-to-fiber diameter ratio, R, by comparing said measured modulation pattern with modulation patterns priorly observed for clad optical fibers of the same core and cladding indices, measured at the same scattering angle range Δθ R ; and then computing said core diameter D C from the equation: D.sub.C = 2Rt/(1 - R).

Claim 5

A method of measuring the cladding thickness, t, of a clad optical fiber of known core diameter, D C and known cladding and core refractive indices m 1 and m 2 , respectively, which comprises: directing a beam of spatially coherent, monochromatic radiation at said fiber thereby to generate a complex scattering pattern, at least a portion of said pattern including contributions from the diffraction, the reflection and the refraction of said beam by said fiber, said scattering pattern being spatially radially disposed about said fiber and having a fringe pattern intensity modulation superimposed thereon; at a given reference angle θ R , measuring the modulation pattern over a scattering angle range Δθ R , where θ R satisfies the relationship: θ.sub.R + 1/2Δθ.sub.R < θ.sub.F where, θ F , the fring cut-off angle satisfies the relation: m.sub.1 cos (θ.sub.F /2) = 1; determining the core-to-fiber diameter ratio, R, by comparing said measured modulation pattern with modulation patterns priorly observed for clad optical fibers of the same core and cladding indices, measured at the same scattering angle range Δθ R ; and then computing said cladding thickness t from the equation: t = D.sub.C (1 - R)/2R.

Claim 6

A method of measuring the cladding thickness, t, of a clad optical fiber of known core diameter, D C and known cladding and core refractive indices m 1 and m 2 , respectively, which comprises: directing a beam of spatially coherent, monochromatic radiation at said fiber thereby to generate a complex scattering pattern, at least a portion of said pattern including contributions from the diffraction, the reflection and the refraction of said beam by said fiber, said scattering pattern being spatially radially disposed about said fiber and having a fringe pattern intensity modulation superimposed thereon; at a given reference angle θ R , measuring the modulation pattern over a scattering angle range Δθ R , where θ R satisfies the relationship: θ.sub.R + 1/2Δθ.sub.R < θ.sub.F where, θ F , the fring cut-off angle satisfies the relation: m.sub.1 cos (θ.sub.F /2) = 1; determining the core-to-fiber diameter ratio, R, by comparing said measured modulation pattern with modulation patterns priorly observed for clad optical fibers of the same core and cladding indices, measured at the same scattering angle range Δθ R ; and then computing said cladding thickness t from the equation: t = D.sub.C (1 - R)/2R.

Claim 9

A method of measuring the degree of noncircularity in a transparent filament, comprising the steps of: a. directing a beam of spatially coherent, monochromatic radiation at said filament thereby to generate a complex scattering pattern, at least a portion of said pattern including contributions from the diffraction, the reflection, and the refraction of said beam by said filament, said scattering pattern being spatially radially disposed about said filament; b. at a given scattering angle θ R , counting the number of fringes N 1 which occur in said pattern over the range Δθ R which range is centered on said given scattering angle, said scattering angle satisfying the relation: θ.sub.R + 1/2Δθ.sub.R < θ.sub.F where, θ F , the fringe cut-off angle satisfies the inequality: m.sub.1 cos (θ.sub.F /2) ≧ 1. and m 1 is a refractive index of the filament; c. repeating step (b) for the given scattering angle -θ R , thereby counting the number of fringes N 2 ; d. computing the difference between N 1 and N 2 ; and then e. determining the degree of non-circularity by comparing said difference with corresponding fringe number differences from priorly measured filaments of the same mean diameter and refractive index.

Claim 10

A method of measuring the degree of noncircularity in a transparent filament, comprising the steps of: a. directing a beam of spatially coherent, monochromatic radiation at said filament thereby to generate a complex scattering pattern, at least a portion of said pattern including contributions from the diffraction, the reflection, and the refraction of said beam by said filament, said scattering pattern being spatially radially disposed about said filament; b. at a given scattering angle θ R , counting the number of fringes N 1 which occur in said pattern over the range Δθ R which range is centered on said given scattering angle, said scattering angle satisfying the relation: θ.sub.R + 1/2Δθ.sub.R < θ.sub.F where, θ F , the fringe cut-off angle satisfies the inequality: m.sub.1 cos (θ.sub.F /2) ≧ 1. and m 1 is a refractive index of the filament; c. repeating step (b) for the given scattering angle -θ R , thereby counting the number of fringes N 2 ; d. computing the difference between N 1 and N 2 ; and then e. determining the degree of non-circularity by comparing said difference with corresponding fringe number differences from priorly measured filaments of the same mean diameter and refractive index.

Claim 11

A method of measuring the deviation from concentricity of the core of a clad optical fiber of known outer diameter and known core and clad refractive indices, comprising the steps of: directing a beam of spatially coherent, monochromatic radiation at said fiber thereby to generate a complex scattering pattern, at least a portion of said pattern including contributions from the diffraction, the reflection, and the refraction of said beam by said fiber, said scattering pattern being spatially radially disposed about said fiber, said pattern having a fringe modulation imposed thereon; measuring θ 1 and θ 2 , the lowest angles at which said modulation first appears in said fringe pattern, where θ 1 < 0 < θ 2 ; and determining the deviation from concentricity by comparing θ 1 and θ 2 with corresponding angles priorly measured for similar clad fibers of known diameter and concentricity and known core and cladding refractive indices.

Claim 12

A method of measuring the deviation from concentricity of the core of a clad optical fiber of known outer diameter and known core and clad refractive indices, comprising the steps of: directing a beam of spatially coherent, monochromatic radiation at said fiber thereby to generate a complex scattering pattern, at least a portion of said pattern including contributions from the diffraction, the reflection, and the refraction of said beam by said fiber, said scattering pattern being spatially radially disposed about said fiber, said pattern having a fringe modulation imposed thereon; measuring θ 1 and θ 2 , the lowest angles at which said modulation first appears in said fringe pattern, where θ 1 < 0 < θ 2 ; and determining the deviation from concentricity by comparing θ 1 and θ 2 with corresponding angles priorly measured for similar clad fibers of known diameter and concentricity and known core and cladding refractive indices.