Method for film thickness and refractive index determination

Claim 1

A method for determining the unknown thickness t, within a predetermined thickness range t min ≦t≦t max , of a film of material with predetermined indices of refraction n 2 =n 2 (λ j ) (j=1,2, . . . , w) at a plurality of w(≧2) distinct wavelengths λ=λ 1 ,λ 2 , . . . , λ w of light used to illuminate the film, where the film material is at least partially transparent to light at each of these wavelengths, where the film is attached on one of its faces to a solid substrate of predetermined material having predetermined indices of refraction n 3 =n 3 (λ j ) at the plurality of wavelengths λ j =λ 1 ,λ 2 , . . . , λ w , where the coefficient of amplitude reflection, for a light beam of polarization index k'(=p,s), incidence angle θ 1 ' and transmission angle θ 2 ' of a light beam of wavelength λ j (j=1,2, . . . , w) traveling in a vacuum toward the interface between the vacuum and the film, is a predetermined number r 12 =r 12 ,k'(θ 1 ', θ 2 '; λ j ) for each of the wavelengths λ j , and where the coefficient of amplitude reflection, for a light beam of polarization index k'(=p, s), incidence angle θ 2 ' and transmission angle θ 3 ' of a light beam of wavelength λ j traveling in the film material toward the interface between the film and the substrate, is a predetermined number r 23 r 23 ,k (θ 2 ', θ 3 '; λ j ), the method comprising the steps of: directing a beam of light of polarization index k(=p, s) at each of the wavelengths λ 1 ,λ 2 , . . . , λ w at a predetermined, nonnegative incidence angle θ 1 at the exposed face of the film within a vacuum or air; measuring the reflectivities R j =R(θ 1 ; λ j ) (j=1,2, . . . , w) of the light beam intensity at the exposed face of the film at incidence angle θ 1 and at each of the respective wavelengths λ 1 ,λ 2 , . . . , λ w ; for each reflectivity number R j determining a thickness t(λ j ) by inverting the equation ##EQU41## to obtain a sequence of w-tuples of film thickness {t m (λ 1 ), t m (λ 2 ), . . . , t m (λ w )} m=1 M (M≧1) that are solutions of this equation, with cos θ.sub.2 =(1-sin.sup.2 θ.sub.1 /n.sub.2 (λ.sub.j).sup.2).sup.1/2, cos θ.sub.3 =(1-sin.sup.2 θ.sub.1 /n.sub.3 (λ.sub.j).sup.2).sup.1/2, r.sub.12 =r.sub.12,k (θ.sub.1, θ.sub.2 ; λ.sub.j), r.sub.23 =r.sub.23,k (θ.sub.2, θ.sub.3 ; λ.sub.j), for the wavelength λ=λ j ; for each w-tuple of thicknesses, determining the statistical means μ t and standard deviation σ t for that w-tuple; and choosing the thickness w-tuple that produces the smallest standard deviation σ t among a sequence of such w-tuples, and designating the mean μ t of that thickness w-tuple as the thickness t of the film.

Claim 2

A method for determining the unknown thickness t, within a predetermined thickness range t min ≦t≦t max , of a film of material with predetermined indices of refraction n 2 =n 2 (λ j ) (j=1,2, . . . , w) at a plurality of w(≧2) distinct wavelengths λ=λ 1 ,λ 2 , . . . , λ w of light used to illuminate the film, where the film material is at least partially transparent to light at each of these wavelengths, where the film is attached on one of its faces to a solid substrate of predetermined material having predetermined indices of refraction n 3 =n 3 (λ j ) at the plurality of wavelengths λ j =λ 1 ,λ 2 , . . . , λ w , where the coefficient of amplitude reflection, for a light beam of polarization index k'(=p,s), incidence angle θ 1 ' and transmission angle θ 2 ' of a light beam of wavelength λ j (j=1,2, . . . , w) traveling in a vacuum toward the interface between the vacuum and the film, is a predetermined number r 12 =r 12 ,k'(θ 1 ', θ 2 '; λ j ) for each of the wavelengths λ j , and where the coefficient of amplitude reflection, for a light beam of polarization index k'(=p, s), incidence angle θ 2 ' and transmission angle θ 3 ' of a light beam of wavelength λ j traveling in the film material toward the interface between the film and the substrate, is a predetermined number r 23 r 23 ,k (θ 2 ', θ 3 '; λ j ), the method comprising the steps of: directing a beam of light of polarization index k(=p, s) at each of the wavelengths λ 1 ,λ 2 , . . . , λ w at a predetermined, nonnegative incidence angle θ 1 at the exposed face of the film within a vacuum or air; measuring the reflectivities R j =R(θ 1 ; λ j ) (j=1,2, . . . , w) of the light beam intensity at the exposed face of the film at incidence angle θ 1 and at each of the respective wavelengths λ 1 ,λ 2 , . . . , λ w ; for each reflectivity number R j determining a thickness t(λ j ) by inverting the equation ##EQU41## to obtain a sequence of w-tuples of film thickness {t m (λ 1 ), t m (λ 2 ), . . . , t m (λ w )} m=1 M (M≧1) that are solutions of this equation, with cos θ.sub.2 =(1-sin.sup.2 θ.sub.1 /n.sub.2 (λ.sub.j).sup.2).sup.1/2, cos θ.sub.3 =(1-sin.sup.2 θ.sub.1 /n.sub.3 (λ.sub.j).sup.2).sup.1/2, r.sub.12 =r.sub.12,k (θ.sub.1, θ.sub.2 ; λ.sub.j), r.sub.23 =r.sub.23,k (θ.sub.2, θ.sub.3 ; λ.sub.j), for the wavelength λ=λ j ; for each w-tuple of thicknesses, determining the statistical means μ t and standard deviation σ t for that w-tuple; and choosing the thickness w-tuple that produces the smallest standard deviation σ t among a sequence of such w-tuples, and designating the mean μ t of that thickness w-tuple as the thickness t of the film.

Claim 4

A method for determining the unknown thickness t, within a predetermined thickness range t min ≦t≦t max , of a film of material with predetermined indices of refraction n 2 =n 2 (λ j ) (j=1,2, . . . , w) at a plurality of w distinct wavelengths λ=λ 1 ,λ 2 , . . . , λ w of light used to illuminate the film, where the film is at least partially transparent to light at each of those wavelengths, where the film is attached on one of its faces to a solid substrate of predetermined material having predetermined indices of refraction n 3 =n 3 (λ j ) at the plurality of wavelengths λ j =λ 1 ,λ 2 , . . . , λ w , where the coefficient of amplitude reflection of a light beam of polarization index k(=p,s) and wavelength λ j that is approaching an interface of vacuum and film within the vacuum at incidence angle θ 1 ' and with transmission angle within the film of θ 2 ' is a predetermined number r 12 =r 12 ,k' (θ 1 ', θ 2 '; λ j ), and where the coefficient of amplitude reflection of a light beam of polarization index k'(=p,s) and wavelength λ j that is approaching an interface of fim and substrate within the film at incidence angle θ 2 ' and with transmission angle θ 3 ' is a predetermined number r 23 =r 23 ,k' (θ 2 ', θ 3 '; λ j ), the method comprising the steps of: directing a beam of light of polarization index k(=p,s ) at each of the wavelengths λ 1 ,λ 2 , . . . , λ w and at a predetermined, nonnegative incidence angle θ 1 at the vacuum-film interface within the vacuum; measuring the total reflectivity R' j =R(θ 1 ; λ j ) (j=1,2, . . . , w) of the film/substrate at incidence angle θ 1 at each of the wavelengths λ j =λ 1 ,λ 2 , . . . , λ w ; choosing an array of film thickness values t 1 ,t 2 , . . . , t M with t min ≦t 1 <t 2 <. . . <t M ≦t max ; generating an array R(θ 1 ; λ j ; t s ) of computed reflectivity numbers for each wavelength λ j =λ 1 ,λ 2 , . . . , λ w and each film thickness t s =t 1 ,t 2 , . . . , t M according to the relation ##EQU45## forming an array of variance numbers ##EQU46## for s=1,2, . . . , M; and choosing as the thickness t of the film the value t s from the array of film thickness values for which the variance x R (t s ) is a minimum.

Claim 5

A method for determining the unknown thickness t, within a predetermined thickness range t min ≦t≦t max , of a film of material with predetermined indices of refraction n 2 =n 2 (λ j ) (j=1,2, . . . , w) at a plurality of w distinct wavelengths λ=λ 1 ,λ 2 , . . . , λ w of light used to illuminate the film, where the film is at least partially transparent to light at each of those wavelengths, where the film is attached on one of its faces to a solid substrate of predetermined material having predetermined indices of refraction n 3 =n 3 (λ j ) at the plurality of wavelengths λ j =λ 1 ,λ 2 , . . . , λ w , where the coefficient of amplitude reflection of a light beam of polarization index k(=p,s) and wavelength λ j that is approaching an interface of vacuum and film within the vacuum at incidence angle θ 1 ' and with transmission angle within the film of θ 2 ' is a predetermined number r 12 =r 12 ,k' (θ 1 ', θ 2 '; λ j ), and where the coefficient of amplitude reflection of a light beam of polarization index k'(=p,s) and wavelength λ j that is approaching an interface of fim and substrate within the film at incidence angle θ 2 ' and with transmission angle θ 3 ' is a predetermined number r 23 =r 23 ,k' (θ 2 ', θ 3 '; λ j ), the method comprising the steps of: directing a beam of light of polarization index k(=p,s ) at each of the wavelengths λ 1 ,λ 2 , . . . , λ w and at a predetermined, nonnegative incidence angle θ 1 at the vacuum-film interface within the vacuum; measuring the total reflectivity R' j =R(θ 1 ; λ j ) (j=1,2, . . . , w) of the film/substrate at incidence angle θ 1 at each of the wavelengths λ j =λ 1 ,λ 2 , . . . , λ w ; choosing an array of film thickness values t 1 ,t 2 , . . . , t M with t min ≦t 1 <t 2 <. . . <t M ≦t max ; generating an array R(θ 1 ; λ j ; t s ) of computed reflectivity numbers for each wavelength λ j =λ 1 ,λ 2 , . . . , λ w and each film thickness t s =t 1 ,t 2 , . . . , t M according to the relation ##EQU45## forming an array of variance numbers ##EQU46## for s=1,2, . . . , M; and choosing as the thickness t of the film the value t s from the array of film thickness values for which the variance x R (t s ) is a minimum.

Claim 6

A method for determining the refractive index n 2 of a film of material from a sequence {r meas .sup.(i) } J=1 Mi (M≧1) of measured values of reflectivity R meas .sup.(i) =R meas (λ; θ 1 ; i; t i ; k i ; n 3 ; θ 3 ) at a sequence of predetermined combinations of film thickness t i , incidence angle θ 1 ,i and beam polarization index k i (=p or s), where each film is mounted on a substrate of known refractive index n 3 =n 3 (λ) and the exposed surface of each film of thickness t i is irradiated by an optical beam of predetermined wavelength λ of beam polarization index k i at incidence angle θ 1 ,i, the method comprising the steps of: choosing a sequence, preferably monotonically increasing or monotonically decreasing, {n 2 ,j } j=1 N of realistic values of the refractive index and computing a corresponding sequence {θ 2 ,j } j=1 N of values of refraction angle θ 2 substantially according to the equation cos θ.sub.2 =[1-sin.sup.2 θ.sub.1 /n.sub.2.sup.2 ].sup.1/2 ; forming the functional values ##EQU47## forming the sums ##EQU48## where h is a predetermined positive real number; determining the integer or integers j=J for which S j =J is the minimum of all values in the sequence {S j } j=1 N ; and choosing n 2 =n 2 ,J as the refractive index of the film.

Claim 7

A method for determining the refractive index n 2 of a film of material from a sequence {r meas .sup.(i) } J=1 Mi (M≧1) of measured values of reflectivity R meas .sup.(i) =R meas (λ; θ 1 ; i; t i ; k i ; n 3 ; θ 3 ) at a sequence of predetermined combinations of film thickness t i , incidence angle θ 1 ,i and beam polarization index k i (=p or s), where each film is mounted on a substrate of known refractive index n 3 =n 3 (λ) and the exposed surface of each film of thickness t i is irradiated by an optical beam of predetermined wavelength λ of beam polarization index k i at incidence angle θ 1 ,i, the method comprising the steps of: choosing a sequence, preferably monotonically increasing or monotonically decreasing, {n 2 ,j } j=1 N of realistic values of the refractive index and computing a corresponding sequence {θ 2 ,j } j=1 N of values of refraction angle θ 2 substantially according to the equation cos θ.sub.2 =[1-sin.sup.2 θ.sub.1 /n.sub.2.sup.2 ].sup.1/2 ; forming the functional values ##EQU47## forming the sums ##EQU48## where h is a predetermined positive real number; determining the integer or integers j=J for which S j =J is the minimum of all values in the sequence {S j } j=1 N ; and choosing n 2 =n 2 ,J as the refractive index of the film.

Claim 8

A method for determining the refractive index n 2 of a material from measured values R meas .sup.(1), R meas .sup.(2), . . . , R meas .sup.(M) of the optical reflectivity of a substantially planar film of the material mounted on a substrate of known material at M≧1 combinations of film thickness and optical beam incidence angle {(t j , θ 1 ,j)} j=1 M for a predetermined optical beam polarization and a predetermined optical beam wavelength λ and known refractive index n 3 (λ) of the substrate material, the method comprising the steps of: choosing an initial estimated value n 2 ,o for the refractive index n 2 ; computing the functional values ##EQU49## forming the sums ##EQU50## determining a new estimate n 2 ,i+1 (i=0,1,2, . . . ) for the film refractive index substantially by the relation ##EQU51## where η≧1 is a predetermined real number; repeating steps 2, 3 and 4 above for i=0,1,2, . . . , I, where i=I is the first positive integer for which |n.sub.2,i+1 -n.sub.2,i |≦ε for a predetermined positive number ε; and choosing n 2 =n 2 ,I+1 as the refractive index of the film.

Claim 9

A method for determining the refractive index n 2 of a material from measured values R meas .sup.(1), R meas .sup.(2), . . . , R meas .sup.(M) of the optical reflectivity of a substantially planar film of the material mounted on a substrate of known material at M≧1 combinations of film thickness and optical beam incidence angle {(t j , θ 1 ,j)} j=1 M for a predetermined optical beam polarization and a predetermined optical beam wavelength λ and known refractive index n 3 (λ) of the substrate material, the method comprising the steps of: choosing an initial estimated value n 2 ,o for the refractive index n 2 ; computing the functional values ##EQU49## forming the sums ##EQU50## determining a new estimate n 2 ,i+1 (i=0,1,2, . . . ) for the film refractive index substantially by the relation ##EQU51## where η≧1 is a predetermined real number; repeating steps 2, 3 and 4 above for i=0,1,2, . . . , I, where i=I is the first positive integer for which |n.sub.2,i+1 -n.sub.2,i |≦ε for a predetermined positive number ε; and choosing n 2 =n 2 ,I+1 as the refractive index of the film.

Claim 10

A method for determining the refractive index n 2 of a material from measured values R meas .sup.(1), R meas .sup.(2), . . ., R meas .sup.(M) of the optical reflectivity of a substantially planar film of the material mounted on a substrate of known material at M≧1 combinations of film thickness and optical beam incidence angle }(t j ,θ 1 ,j)} j=1 M for a predetermined optical beam polarization and a predetermined optical beam wavelength λ and known refractive index n 3 (λ) of the substrate material, the method comprising the steps of: choosing an initial estimated value n 2 ,o for the refractive index n 2 ; computing the functional values ##EQU52## determining a new estimate n 2 ,i +1 (i=0,1,2, . . . ) for the film refractive index substantially by the relation ##EQU53## where η≧1 is a predetermined real number; repeating steps 2, 3 and 4 above for i=0,1,2, . . . , I, where i=I is the first positive integer for which |n.sub.2,i+1 -n.sub.2,i |≦ε for a predetermined positive number ε; and choosing n 2 =n 2 ,I+1 as the refractive index of the film.

Claim 11

A method for determining the refractive index n 2 of a material from measured values R meas .sup.(1), R meas .sup.(2), . . ., R meas .sup.(M) of the optical reflectivity of a substantially planar film of the material mounted on a substrate of known material at M≧1 combinations of film thickness and optical beam incidence angle }(t j ,θ 1 ,j)} j=1 M for a predetermined optical beam polarization and a predetermined optical beam wavelength λ and known refractive index n 3 (λ) of the substrate material, the method comprising the steps of: choosing an initial estimated value n 2 ,o for the refractive index n 2 ; computing the functional values ##EQU52## determining a new estimate n 2 ,i +1 (i=0,1,2, . . . ) for the film refractive index substantially by the relation ##EQU53## where η≧1 is a predetermined real number; repeating steps 2, 3 and 4 above for i=0,1,2, . . . , I, where i=I is the first positive integer for which |n.sub.2,i+1 -n.sub.2,i |≦ε for a predetermined positive number ε; and choosing n 2 =n 2 ,I+1 as the refractive index of the film.

Claim 12

A method for determining the refractive index n 2 of a φ=4 πt/λ; reflectivity at a predetermined wavelength λ of a substantially planar film of known film thickness t of the material, mounted on a substantially planar substrate of known substrate refractive index n 3 (λ), the method comprising the steps of: irradiating the exposed surface of the film with an optical beam of s-wave beam polarization and wavelength λ at a predetermined incidence angle θ 1 and measuring the reflectivity R meas of the film; forming the ratios ψ 13 =cos θ 1 /[n 3 (λ) 2 -sin 2 θ 1 ], and θ=4ρt/λ; solving the equation ##EQU54## for all real positive roots z in a predetermined interval on the positive real axis; and determining n 2 substantially as n.sub.2 =[(z cos θ.sub.1).sup.2 +sin.sup.2 θ.sub.1 ].sup.1/2.

Claim 13

A method for determining the refractive index n 2 of a φ=4 πt/λ; reflectivity at a predetermined wavelength λ of a substantially planar film of known film thickness t of the material, mounted on a substantially planar substrate of known substrate refractive index n 3 (λ), the method comprising the steps of: irradiating the exposed surface of the film with an optical beam of s-wave beam polarization and wavelength λ at a predetermined incidence angle θ 1 and measuring the reflectivity R meas of the film; forming the ratios ψ 13 =cos θ 1 /[n 3 (λ) 2 -sin 2 θ 1 ], and θ=4ρt/λ; solving the equation ##EQU54## for all real positive roots z in a predetermined interval on the positive real axis; and determining n 2 substantially as n.sub.2 =[(z cos θ.sub.1).sup.2 +sin.sup.2 θ.sub.1 ].sup.1/2.