Refractive index measurement method, measurement apparatus, and optical element manufacturing method
US-2016363531-A1 · Dec 15, 2016 · US
US10823636B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-10823636-B2 |
| Application number | US-201816223719-A |
| Country | US |
| Kind code | B2 |
| Filing date | Dec 18, 2018 |
| Priority date | Dec 21, 2017 |
| Publication date | Nov 3, 2020 |
| Grant date | Nov 3, 2020 |
A practical reading order for non-experts. Skip the full description unless you need deep technical detail.
What the patent document calls the invention.
A short plain-language summary of the technical disclosure.
Who owns or filed the patent and who is credited as inventor.
Filing, priority, publication, and grant dates set the timeline.
The legal scope of protection — read this for what is actually claimed.
Technology tags used to group this patent with similar filings.
Prior art links and similar publications in this corpus.
Official abstract text for this publication.
Method for determining the refractive index (n) of a material of a contact lens, in particular of a soft contact lens, the contact lens (1) having a first surface and a second surface defining a lens geometry there between, by measuring the wavefront issued by the contact lens (1) with a wavefront sensor (4), obtaining data of the geometry of at least one section of the contact lens (1) with an optical coherence tomography system (3) and communicating the geometry of the at least one section of the contact lens (1) from the optical coherence tomography system (3) to an analyzer, particularly a computer, and determining the refractive index (n) of the material of the contact lens from the geometry of the at least one section of the contact lens and from the wavefront issued by the contact lens (1).
Opening claim text (preview).
The invention claimed is: 1. A method for determining the refractive index (n) of a material of a contact lens ( 1 ), the contact lens ( 1 ) having a first surface and a second surface defining a lens geometry there between, the method comprising the steps of: a) providing a lens holder ( 2 ) comprising an optically transparent bottom ( 21 ) and containing the contact lens ( 1 ), b) providing a wavefront sensor ( 4 ), the wavefront sensor ( 4 ) comprising a light source ( 40 ) and a detector ( 43 ) for receiving light coming from the light source ( 40 ) and having passed through the contact lens ( 1 ) contained in the lens holder ( 2 ) and impinging on the detector ( 43 ), thus generating signals at the detector ( 43 ) measuring the wavefront issued by the contact lens ( 1 ) with the wavefront sensor ( 4 ), c) providing an optical coherence tomography system ( 3 ) and obtaining data of a geometry of at least one section of the contact lens ( 1 ) with the optical coherence tomography system ( 3 ), d) communicating the measured wavefront from the wavefront sensor ( 4 ) and the data of the geometry of the at least one section of the contact lens from the optical coherence tomography system ( 3 ) to an analyzer ( 5 ), e) determining the refractive index (n) of the material of the contact lens from the data of the geometry of the at least one section (S) of the contact lens ( 1 ) and from the wavefront issued by the contact lens ( 1 ). wherein determining the refractive index (n) of the material of the contact lens in step e) comprises the steps of: e1) obtaining the three dimensional geometry of the at least one section of the contact lens ( 1 ) by performing a calculation using an approximation of the refractive index (n), e2) calculating the theoretical wavefront of the light passing through the contact lens in the at least one section of the contact lens ( 1 ) on basis of the three dimensional geometry of the at least one section of the contact lens ( 1 ) obtained in step el) using a wavefront simulation, e3) comparing the theoretical wavefront obtained in step e2) and the measured wavefront obtained in step b) in the at least one section and calculating a parameter of deviation of the theoretical wave front from the measured wavefront in the at least one section (S) of the contact lens ( 1 ), the parameter of deviation being an indication of the accuracy of the determined refractive index (n), e4) incrementally adjusting the approximated refractive index (n) and reiterating the steps e1) to e3) until the parameter of deviation passes a predetermined threshold value. 2. The method according to claim 1 , wherein in step e) a three dimensional geometry of the at least one section of the contact lens ( 1 ) is obtained from the data of the geometry from the optical coherence tomography system and an approximated refractive index (n) of the material of the contact lens, for determining the refractive index (n), wherein determining the refractive index (n) of the material of the contact lens in step e) comprises the steps of: e1) obtaining the three dimensional geometry of the at least one section of the contact lens ( 1 ) by performing a calculation using an approximation of the refractive index (n), e2) calculating the theoretical wavefront of the light passing through the contact lens in the at least one section of the contact lens ( 1 ) on basis of the three dimensional geometry of the at least one section of the contact lens ( 1 ) obtained in step e1) using a wavefront simulation, e3) comparing the theoretical wavefront obtained in step e2) and the measured wavefront obtained in step b) in the at least one section and calculating a parameter of deviation of the theoretical wave front from the measured wavefront in the at least one section (S) of the contact lens ( 1 ), the parameter of deviation being an indication of the accuracy of the determined refractive index (n), e4) incrementally adjusting the approximated refractive index (n) and reiterating the steps e1) to e3) until the parameter of deviation passes a predetermined threshold value. 3. An apparatus for determining a refractive index (n) of a material of a contact lens ( 1 ), the apparatus comprising: a) an optical coherence tomography system ( 3 ) configured to obtain data of a geometry of the contact lens ( 1 ); b) a wavefront sensor ( 4 ) comprising a light source ( 40 ) and a sensor array ( 43 ), the light source ( 40 ) being configured to emit a beam of light ( 41 ) which is directed through the contact lens ( 1 ) and onto the sensor array ( 43 ), the wavefront sensor ( 4 ) being adapted to measure a wavefront of the light beam ( 41 ) having passed through the contact lens ( 1 ), and c) an analyzer ( 5 ), configured to determine the refractive index (n) of the material of the contact lens from the data of the geometry of the contact lens ( 1 ) and from the wavefront of the light beam having passed through the contact lens ( 1 ), wherein the analyzer ( 5 ) is configured to determine the refractive index (n) of the material of the contact lens ( 1 ) by i) obtaining a three dimensional geometry of the at least one section of the contact lens ( 1 ) by performing a calculation using an approximation of the refractive index (n), ii) calculating the theoretical wavefront of the light having passed through the contact lens ( 1 ) in the at least one section of the contact lens ( 1 ) using a simulation on basis of the three dimensional geometry of at least one section of the contact lens ( 1 ) obtained in step i), iii) comparing the theoretical wavefront obtained in step i) and the measured wavefront obtained in step b) and calculating a parameter of deviation of the calculated wave front from the measured wavefront in the at least one section of the contact lens ( 1 ), the parameter of deviation being an indication of the accuracy of the determined refractive index (n), and iv) incrementally adjusting the approximated refractive index (n) and reiterating the steps i) to iii) until the parameter of deviation passes a predetermined threshold value. 4. The apparatus according to claim 3 , wherein the wavefront sensor is a Shack-Hartmann wavefront sensor ( 4 ) comprising a plurality of lenslets ( 42 ) placed in front of the sensor array ( 43 ) and wherein the beam of light ( 41 ) is directed through the contact lens ( 1 ), through the plurality of lenslets ( 42 ), and onto the sensor array ( 43 ).
Tomographic interferometers, e.g. based on optical coherence · CPC title
Lenses · CPC title
using interferometric methods; using Schlieren methods · CPC title
using interferometry · CPC title
Contact lenses for the eyes (disinfection or sterilisation of contact lenses A61L12/00) · CPC title
Related publications grouped by family.
Answers are generated from the same data shown on this page.