Low thermal stress birefringence imaging lens
AssigneeEastman Kodak Company
InventorsAndrew F. Kurtz, Joseph Raymond Bietry, Barry David Silverstein
Life of this patent
Estimating the term…
Abstract
An imaging lens having reduced susceptibility to thermally-induced stress birefringence for imaging an object plane to an image plane; comprising a plurality of lens elements. The lens element that experiences a highest optical power density is fabricated using a glass having a negligible susceptibility to thermal stress birefringence as characterized by the thermal stress birefringence metric. The other lens elements are fabricated using glasses having a negligible or a moderate susceptibility to thermal stress birefringence, at least one of the other lens elements being fabricated using a glass having a moderate susceptibility to thermal stress birefringence.
Claims17
A lens system having reduced susceptibility to thermally-induced stress birefringence for imaging an object plane onto an image plane comprising;
- a plurality of lens elements arranged to image the object plane onto the image plane,
- wherein the lens element that experiences a highest optical power density from transiting light when the lens system is used to image the object plane onto the image plane is fabricated using a glass having a negligible susceptibility to thermal stress birefringence as characterized by a thermal stress birefringence metric;
- wherein the other lens elements are fabricated using glasses having a negligible or a moderate susceptibility to thermal stress birefringence as characterized by the thermal stress birefringence metric, at least one of the other lens elements being fabricated using a glass having a moderate susceptibility to thermal stress birefringence;
- wherein the thermal stress birefringence metric has the form:
- M1=ρκαE/(K·(1−μ).
- where ρ is a coefficient of thermal expansion of the glass, κ is a stress optical coefficient of the glass, α is a light absorption coefficient of the glass, E is a modulus of elasticity of the glass, K is a thermal conductivity of the glass, and μ is a Poisson's ratio of the glass;
- and
- wherein the glasses having the negligible susceptibility to thermal stress birefringence satisfy the condition that M1≦0.1×10−6 W−1 and the glasses having the moderate susceptibility to thermal stress birefringence satisfy the condition that 0.1×10−6 W−1≦M1<1.6×10−6 W−1.
A lens system having reduced susceptibility to thermally-induced stress birefringence for imaging an object plane onto an image plane comprising;
- a plurality of lens elements arranged to image the object plane onto the image plane;
- wherein the lens element that experiences a highest optical power density from transiting light when the lens system is used to image the object plane onto the image plane is fabricated using a glass having a negligible susceptibility to thermal stress birefringence as characterized by a thermal stress birefringence metric;
- wherein the other lens elements are fabricated using glasses having a negligible or a moderate susceptibility to thermal stress birefringence as characterized by the thermal stress birefringence metric, at least one of the other lens elements being fabricated using a glass having a moderate susceptibility to thermal stress birefringence;
- wherein the thermal stress birefringence metric is given by:
- M1′=ρκα.
- where ρ is the coefficient of thermal expansion, κ is the stress optical coefficient, and α is the light absorption coefficient;
- and
- wherein the glasses having the negligible susceptibility to thermal stress birefringence satisfy the condition that M1′≦0.0008×10−12 mm/(N K) and the glasses having the moderate susceptibility to thermal stress birefringence satisfy the condition that 0.0008×10−12 mm/(N K)≦M1′≦0.01×10−12 mm/(N K).
Dependencies are inferred from the claim text.