IP Library Granted Patent US 7,324,281
Granted Patent B2
US 7,324,281 · App. 11/607,521 · Granted Jan 29, 2008

Refractive boundary elements, devices, and materials

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Quick Facts
Patent No.
US 7,324,281
App. No.
11/607,521
Granted
Jan 29, 2008
Kind
B2
Abstract

An optical device includes an interface between two or more media. The refractive indices, orientations of media, and alignment relative to a propagating wave define a refractive boundary at which reflections may be reduced or eliminated, and at which, for certain incident angles, rays may be refracted on the same side of the normal as the incident ray.

Claims (60)

1. An optical element, comprising:

a first layer of a first anisotropic material having a first surface, the first layer having a first optical index of refraction corresponding to a first internal axis and a second optical index of refraction corresponding to a second internal axis, the first and second indices being different, the first anisotropic material being biaxial; and

a second layer of a second material different from the first anisotropic material and having a second surface in intimate contact with the first surface, the second layer having a third optical index of refraction that is a geometric mean of the first and second optical indices of refraction,

wherein the second material is rotated relative to the first anisotropic material, and

wherein the first anisotropic material and second material are materials having principal material axes, and wherein the angle of rotation of the second material relative to the first anisotropic material substantially satisfies the relationship:

β

1

ɛ

1

2

=

β

2

ɛ

2

2

β

1

cos

2

ϕ

1

+

1

β

1

sin

2

ϕ

1

=

β

2

cos

2

ϕ

2

+

1

β

2

sin

2

ϕ

2

where:

ε 1 is a dielectric constant of the first anisotropic material relative to its principal material axis; ε 2 is a dielectric constant of the second material relative to its principal material axis;

β 1 ε 1 is a dielectric constant of the first anisotropic material relative to a second material axis of the first material; β 2 ε 2 is a dielectric constant of the second material relative to a second material axis of the second material; and

φ 1 is an orientation angle of the principal material axis of the first anisotropic material and φ 2 is an orientation angle of the principal material axis of the second material, φ 2 is defined relative to a normal angle to the second surface.

2. The optical element of claim 1 wherein the plane defined by the principal and second material axes of the first material and the plane defined by the principal and second material axes of the second material are in parallel.

Assignments (3)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Sep 19, 2023
From: DEEP SCIENCE LLC
To: ENTERPRISE SCIENCE FUND, LLC
Reel/Frame 064953/0040 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Jan 15, 2016
From: THE INVENTION SCIENCE FUND I, LLC
To: DEEP SCIENCE, LLC
Reel/Frame 037540/0628 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Nov 6, 2009
From: SEARETE LLC
To: INVENTION SCIENCE FUND I
Reel/Frame 023484/0687 →