Process for forming two different indices of refraction in a glass ceramic
AssigneeOwens-Illinois, Inc.
InventorJames E. Rapp
Life of this patent
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Abstract
Thermally crystallizable glasses of the Na.sub.2 O--Ta.sub.2 O.sub.5 --SiO.sub.2 and the Na.sub.2 O--Li.sub.2 O--Ta.sub.2 O.sub.5 --SiO.sub.2 systems, and glass-ceramics made therefrom which are highly transparent, have high indices of refraction, and excellent strength properties. By varying the heat treatment schedule for crystallization of a glass to a glass-ceramic, a specific high index of refraction coming within a prescribed range may be imparted to the finished, transparent glass-ceramic. A transparent glass-ceramic having two or more different indices of refraction may also be produced.
Claims6
A method for forming a transparent glass-ceramic body having at least two different indices of refraction for light transmittal therethrough, said glass-ceramic body being formed by thermally in situ crystallizing a thermally crystallizable glass body, comprising:
- a. heating a first portion of said glass body for a period of time and at a temperature sufficient to nucleate and crystallize said first portion of said glass body to a transparent glass-ceramic having a first index of refraction;
- and
- b. heating a second and different portion of the same glass body for a period of time and at a temperature sufficient to nucleate and crystallize said second portion to a transparent glass-ceramic having a second index of refraction which is different from said first index of refraction.
A method of forming a transparent glass-ceramic body having at least two different indices of refraction comprising the steps of:
- a. forming a thermally crystallizable glass body of a predetermined shape;
- b. heating a first portion of said glass body at an elevated temperature and for a period of time sufficient to thermally in situ crystallize said first portion of said glass body to a transparent glass-ceramic having a first index of refraction;
- c. heating a second and different portion of the same glass body at an elevated temperature and for a period of time sufficient to thermally in situ crystallize said second portion to a transparent glass-ceramic having a second index of refraction which is different from the first index of refraction.
A method of forming a transparent glass-ceramic body having a concentric index of refraction gradient in said body, wherein said transparent glass-ceramic is formed by thermal in situ crystallization of a thermally crystallizable glass body, comprising heating concentric portions of a specific glass body at different elevated temperatures for a period of time sufficient to thermally in situ crystallize said concentric portions of said specific glass body to different transparent concentric glass-ceramic portions of the resulting glass-ceramic body having different indices of refraction.
A method of forming a desired optical path in a thermally crystallizable transparent glass body comprising heating a localized portion of said glass body in a desired configuration defining a path for a period of time and at an elevated temperature sufficient to thermally in situ crystallize said portion of said same glass body defining said path and thus crystallizing said path to a transparent glass-ceramic having an index of refraction which is higher than the index of refraction of the surrounding material, whereby light can be made to follow said path of higher index of refraction transparent glass-ceramic.
A method of forming an optical path in a thermally crystallizable transparent glass block for passage of light along said path comprising heating a portion within said block by directing a laser beam to that portion for a period of time sufficient to form a thermally in situ crystallized transparent glass-ceramic portion and moving said laser beam along said block to heat consecutive adjacent portions of said glass block to thermally in situ crystallize said portions to transparent glass-ceramic portions, said glass-ceramic portions having an index of refraction higher than the index of refraction of said glass surrounding said glass-ceramic portions and defining a continuous optical path for movement of light through said glass-ceramic portions.
Dependencies are inferred from the claim text.