Method of measuring refractive index profile of cylinder

Claim 1

A method of measuring refractive index profile of a cylinder, comprising steps of: applying k distinct parallel rays of light to the cylinder so that the rays enter the cylinder at incident positions P 1 , P 2 , . . . , P k and leave the cylinder at true exit positions Q 1 , Q 2 , . . . , Q k , said rays being on one plane perpendicular to longitudinal axis of said cylinder; measuring said true exit positions; assuming a mathematical function representing a phantom refractive index profile of the cylinder on said plane; calculating phantom exit positions Q 1 ', Q 2 ', . . . , Q k ' for the parallel rays from said incident positions based on said assumed mathematical functions; modifying said mathematical function so as to minimize a sum of the squared distances between the true and phantom exit positions for the rays from said incident positons, wherein said mathematical function is in the form of F(r, a.sub.1, a.sub.2, . . . , a.sub.m), r being distance from an arbitrary point to the longitudinal axis f of the cylinder, a 1 through a m being parameters representing pattern of the refractive index profile of the cylinder, the number m of the parameters being not greater the number k of the rays (k≧m), whereby the thus modified function represents the refractive index profile of the cylinder.

Claim 2

A method of measuring refractive index profile of a cylinder, comprising steps of: applying k distinct parallel rays of light to the cylinder so that the rays enter the cylinder at incident positions P 1 , P 2 , . . . , P k and leave the cylinder at true exit positions Q 1 , Q 2 , . . . , Q k , said rays being on one plane perpendicular to longitudinal axis of said cylinder; measuring said true exit positions; assuming a mathematical function representing a phantom refractive index profile of the cylinder on said plane; calculating phantom exit positions Q 1 ', Q 2 ', . . . , Q k ' for the parallel rays from said incident positions based on said assumed mathematical functions; modifying said mathematical function so as to minimize a sum of the squared distances between the true and phantom exit positions for the rays from said incident positons, wherein said mathematical function is in the form of F(r, a.sub.1, a.sub.2, . . . , a.sub.m), r being distance from an arbitrary point to the longitudinal axis f of the cylinder, a 1 through a m being parameters representing pattern of the refractive index profile of the cylinder, the number m of the parameters being not greater the number k of the rays (k≧m), whereby the thus modified function represents the refractive index profile of the cylinder.

Claim 3

A method of measuring refractive index profile of a cylinder, comprising steps of: applying k distinct parallel rays of light to the cylinder so that the rays enter the cylinder at incident positions P 1 , P 2 , . . . , P k and leave the cylinder at true exit positions Q 1 , Q 2 , . . . , Q k , said rays being on one plane perpendicular to longitudinal axis of said cylinder; measuring said true exit positions; assuming a mathematical function representing a phantom refractive index profile of the cylinder on said plane; calculating phantom exit positions Q 1 ', Q 2 ', . . . , Q k ' for the parallel rays from said incident positions based on said assumed mathematical function; modifying said assumed mathematical function so as to minimize a sum of the squared distances between the true and phantom exit positions for the rays from said incident positions, wherein said mathematical function is in a form of n(r, n.sub.0, g)=n.sub.0 √1-(gr).sup.2, n being refractive index, n 0 being refractive index at the longitudinal axis of the cylinder, r being distance from an arbitrary point in the cylinder to said longitudinal axis of the cylinder, and g being a focusing constant, whereby the thus modified mathematical function represents the refractive index profile of the cylinder.

Claim 4

A method of measuring refractive index profile of a cylinder, comprising steps of: applying k distinct parallel rays of light to the cylinder so that the rays enter the cylinder at incident positions P 1 , P 2 , . . . , P k and leave the cylinder at true exit positions Q 1 , Q 2 , . . . , Q k , said rays being on one plane perpendicular to longitudinal axis of said cylinder; measuring said true exit positions; assuming a mathematical function representing a phantom refractive index profile of the cylinder on said plane; calculating phantom exit positions Q 1 ', Q 2 ', . . . , Q k ' for the parallel rays from said incident positions based on said assumed mathematical function; modifying said assumed mathematical function so as to minimize a sum of the squared distances between the true and phantom exit positions for the rays from said incident positions, wherein said mathematical function is in a form of n(r, n.sub.0, g)=n.sub.0 √1-(gr).sup.2, n being refractive index, n 0 being refractive index at the longitudinal axis of the cylinder, r being distance from an arbitrary point in the cylinder to said longitudinal axis of the cylinder, and g being a focusing constant, whereby the thus modified mathematical function represents the refractive index profile of the cylinder.

Claim 5

A method of measuring refractive index profile of a cylinder, comprising steps of: applying k distinct parallel rays of light to the cylinder so that the rays enter the cylinder at incident positions P 1 , P 2 , . . . , P k and leave the cylinder at true exit positions Q 1 , Q 2 , . . . , Q k , said rays being on one plane perpendicular to longitudinal axis of said cylinder; measuring said true exit positions; assuming a mathematical function representing a phantom refractive index profile of the cylinder on said plane; calculating phantom exit positions Q 1 ', Q 2 ', . . . , Q k ' for the parallel rays from said incident positions based on said assumed mathematical function; modifying said mathematical function so as to minimize sum of squared distances between the true and phantom exit positions for the rays from said incident positions; shifting said plane in the longitudinal direction of the cylinder while keeping the plane perpendicular to said longitudinal axis; and, determining a refractive index profile on the thus moved plane, whereby the thus modified mathematical function represents the refractive index profile of the cylinder and the refractive index profile in the longitudinal direction of the cylinder is measured.

Claim 6

A method of measuring refractive index profile of a cylinder, comprising steps of: applying k distinct parallel rays of light to the cylinder so that the rays enter the cylinder at incident positions P 1 , P 2 , . . . , P k and leave the cylinder at true exit positions Q 1 , Q 2 , . . . , Q k , said rays being on one plane perpendicular to longitudinal axis of said cylinder; measuring said true exit positions; assuming a mathematical function representing a phantom refractive index profile of the cylinder on said plane; calculating phantom exit positions Q 1 ', Q 2 ', . . . , Q k ' for the parallel rays from said incident positions based on said assumed mathematical function; modifying said mathematical function so as to minimize sum of squared distances between the true and phantom exit positions for the rays from said incident positions; shifting said plane in the longitudinal direction of the cylinder while keeping the plane perpendicular to said longitudinal axis; and, determining a refractive index profile on the thus moved plane, whereby the thus modified mathematical function represents the refractive index profile of the cylinder and the refractive index profile in the longitudinal direction of the cylinder is measured.

Claim 7

A method of measuring refractive index profile of a cylinder, comprising steps of: applying k distinct parallel rays of light to the cylinder so that the rays enter the cylinder at incident positions P 1 , P 2 , . . . , P k and leave the cylinder at true exit positions Q 1 , Q 2 , . . . , Q k , said rays being on one plane perpendicular to longitudinal axis of said cylinder measuring said true exit positions; assuming a mathematical function representing a phantom refractive index profile of the cylinder on said plane; calculating phantom exit positions Q 1 ', Q 2 ', . . . , Q k ' for the parallel rays from said incident positions based on said assumed mathematical function; modifying said mathematical function so as to minimize sum of squared distances between the true and phantom exit positions for the rays from said incident positions; shifting said plane in the longitudinal direction of the cylinder while keeping the plane perpendicular to said longitudinal axis; and, determining a refractive index profile on the thus moved plane, wherein said mathematical function is in a form of F(r, a.sub.1, a.sub.2, . . . , a.sub.m), r being distance from an arbitrary point to the longitudinal axis of the cylinder, a 1 through a m being parameters representing pattern of the refractive index profile of the cylinder, the number m of the parameters being not greater the number k of the rays (k≧m), whereby the thus modified function represents the refractive index profile of the cylinder, and the refractive index profile in the longitudinal direction of the cylinder is measured.

Claim 8

A method of measuring refractive index profile of a cylinder, comprising steps of: applying k distinct parallel rays of light to the cylinder so that the rays enter the cylinder at incident positions P 1 , P 2 , . . . , P k and leave the cylinder at true exit positions Q 1 , Q 2 , . . . , Q k , said rays being on one plane perpendicular to longitudinal axis of said cylinder measuring said true exit positions; assuming a mathematical function representing a phantom refractive index profile of the cylinder on said plane; calculating phantom exit positions Q 1 ', Q 2 ', . . . , Q k ' for the parallel rays from said incident positions based on said assumed mathematical function; modifying said mathematical function so as to minimize sum of squared distances between the true and phantom exit positions for the rays from said incident positions; shifting said plane in the longitudinal direction of the cylinder while keeping the plane perpendicular to said longitudinal axis; and, determining a refractive index profile on the thus moved plane, wherein said mathematical function is in a form of F(r, a.sub.1, a.sub.2, . . . , a.sub.m), r being distance from an arbitrary point to the longitudinal axis of the cylinder, a 1 through a m being parameters representing pattern of the refractive index profile of the cylinder, the number m of the parameters being not greater the number k of the rays (k≧m), whereby the thus modified function represents the refractive index profile of the cylinder, and the refractive index profile in the longitudinal direction of the cylinder is measured.

Claim 9

A method of measuring refractive index profile of a cylinder, comprising steps of: applying k distinct parallel rays of light to the cylinder so that the rays enter the cylinder at incident positions P 1 , P 2 , . . . , P k and leave the cylinder at true exit positions Q 1 , Q 2 , . . . , Q k , said rays being on one plane perpendicular to longitudinal axis of said cylinder; measuring said true exit positions; assuming a mathematical function representing a phantom refractive index profile of the cylinder on said plane; calculating phantom exit positions Q 1 ', Q 2 ', . . . , Q k ' for the parallel rays from said incident positions based on said assumed mathematical function; modifying said mathematical function so as to minimize sum of squared distances between the true and phantom exit positions for the rays from said incident positions; shifting said plane in the longitudinal direction of the cylinder while keeping the plane perpendicular to said longitudinal axis; and, determining a refractive index profile on the thus moved plane, wherein said mathematical function is in a form of n(r, n.sub.0, g)=n.sub.0 √1-(gr).sup.2, n being refractive index, n 0 being refractive index at the longitudinal axis of the cylinder, r being distance from an arbitrary point in the cylinder to said longitudinal axis of the cylinder, and g being a focussing constant, whereby the thus modified function represents the refractive index profile of the cylinder and the refractive index profile in the longitudinal direction of the cylinder is measured.

Claim 10

A method of measuring refractive index profile of a cylinder, comprising steps of: applying k distinct parallel rays of light to the cylinder so that the rays enter the cylinder at incident positions P 1 , P 2 , . . . , P k and leave the cylinder at true exit positions Q 1 , Q 2 , . . . , Q k , said rays being on one plane perpendicular to longitudinal axis of said cylinder; measuring said true exit positions; assuming a mathematical function representing a phantom refractive index profile of the cylinder on said plane; calculating phantom exit positions Q 1 ', Q 2 ', . . . , Q k ' for the parallel rays from said incident positions based on said assumed mathematical function; modifying said mathematical function so as to minimize sum of squared distances between the true and phantom exit positions for the rays from said incident positions; shifting said plane in the longitudinal direction of the cylinder while keeping the plane perpendicular to said longitudinal axis; and, determining a refractive index profile on the thus moved plane, wherein said mathematical function is in a form of n(r, n.sub.0, g)=n.sub.0 √1-(gr).sup.2, n being refractive index, n 0 being refractive index at the longitudinal axis of the cylinder, r being distance from an arbitrary point in the cylinder to said longitudinal axis of the cylinder, and g being a focussing constant, whereby the thus modified function represents the refractive index profile of the cylinder and the refractive index profile in the longitudinal direction of the cylinder is measured.