Light emitting diode with integral parabolic reflector

• US 20070019413A1
• Filed: 07/14/2006
• Published: 01/25/2007
• Est. Priority Date: 07/14/2005
• Status: Abandoned Application

• Current Assignee: Playhard Incorporated
• Original Assignee: Playhard Incorporated
• Inventors: Moore, Jerry, Moore, Christian
• Application Number:
  US11/486,921
• Publication Number:
  US 20070019413A1
• Time in Patent Office: Days
• US Class Current: 362/296.80
• CPC Class Codes: H01L 2224/48247 connecting the wire to a bond pad of the item
• CPC Class Codes: H01L 2924/1815 Shape
• CPC Class Codes: H01L 33/54 having a particular shape

Abstract

The dielectric casing of a light emitting diode (LED) incorporates an integral parabolic reflector system which redirects light in a collimated pattern deflected at significant angles relative to the axis of symmetry of the LED.

Claims

1. A light emitting diode (LED) assembly comprising:

a dielectric casing of optically transparent material;

first and second electrical leads extending within said dielectric casing;

at least one semiconductor die embedded in said dielectric casing and coupled to said first and second leads in a manner allowing for transfer of electrical energy to and illumination of said at least one semiconductor die; and

wherein said dielectric casing has a surface, at least a portion of which is parabolic, said parabolic surface portion located and dimensioned for reflecting light emitted by said at least one semiconductor die.

2. An LED assembly as in claim 1 wherein said dielectric casing has a plurality of said parabolic surface portions.

3. An LED assembly as in claim 1 wherein said parabolic surface portion defines a parabolic curve rotated around the axis of said LED.

4. An LED assembly as in claim 1 wherein said parabolic surface portion defines a parabolic curve rotated around an axis through said LED and perpendicular to the axis of said LED.

5. An LED assembly as in claim 1 wherein said parabolic surface portion is located and dimensioned to reflect light emitted by said at least one semiconductor die into a region defining a disc perpendicular to the axis of said LED.

6. An LED assembly as in claim 2 wherein said parabolic surfaces are located and dimensioned to reflect light emitted by said at least one semiconductor die into a plurality of beams.

7. An LED assembly as in claim 1 wherein said dielectric casing has an index of refraction greater than 1.42.

8. A method of directing light in a light emitting diode (LED) assembly, said method comprising:

emitting light from a semiconductor die embedded in a dielectric casing; and

reflecting said emitted light from a parabolic surface portion of said dielectric casing.

9. A method as in claim 8 wherein said reflecting comprises reflecting said light into a region in the form of a disc perpendicular to the axis of said LED.

10. A method as in claim 8 wherein said reflecting comprises reflecting said emitted light from a plurality of said parabolic surface portions.

11. A light emitting diode (LED) assembly having an integral reflector comprising:

a dielectric casing of optically transparent material;

first and second electrical leads extending within said dielectric casing; and

at least one semiconductor die embedded in said dielectric casing and coupled to said first and second leads in a manner allowing for transfer of electrical energy to and illumination of said at least one semiconductor die;

wherein said dielectric casing includes an integral concavity substantially opposite said at least one semiconductor die, the concavity being shaped and dimensioned for reflecting light emitted by said at least one semiconductor die;

wherein said concavity forms a truncated cone whose surface is described by revolving around the symmetric axis of said LED a parabolic segment defined by the equation y²=2Px, P representing a constant scale factor, the parabolic segment having its focus coincident with the centroid of said at least one semiconductor die and its vertex coincident with a line representing the x-axis passing through said centroid, the angle between said x-axis and said LED axis of symmetry determining the deflection angle of the reflector and being greater than 0° and

less than 180°

; and

wherein reflection at said parabolic surface occurs by means of total internal reflection according to Snell'"'"'s Law as expressed by the equation sin θ

_c=n₁/n₂, θ

_c representing the critical minimum angle of incidence beyond which a ray striking the parabolic surface will be totally reflected, n₁, representing the refractive index of air, and n₂ representing the refractive index of said dielectric casing.

12. A light emitting diode (LED) assembly having multiple integral reflectors, said assembly comprising:

a dielectric casing of optically transparent material;

first and second electrical leads extending within said dielectric casing; and

at least one semiconductor die embedded in said dielectric casing and coupled to said first and second leads in a manner allowing for transfer of electrical energy to and illumination of said at least one semiconductor die;

wherein said dielectric casing includes a multiplicity of convex surfaces substantially opposite said at least one semiconductor die, the convex surfaces shaped and dimensioned for reflecting light emitted by said at least one semiconductor die;

wherein each said convex surface has an associated x-axis which passes through the centroid of said at least one semiconductor die; and

each said convex surface forms a truncated cone as described by revolving around said associated x-axis a parabolic segment defined by the equation y²=2Px, P representing a constant scale factor, said parabolic segment having its focus coincident with the centroid of said at least one semiconductor die and its vertex coincident with said associated x-axis, the angle between said associated x-axis and the LED axis of symmetry determining the deflection angle of the reflector and being greater than 0° and

less than 180°

; and

wherein reflection at said parabolic surface occurs by means of total internal reflection according to Snell'"'"'s Law as expressed bythe equation sin θ

_c=n₁/n₂, θ

_c representing the critical minimum angle of incidence beyond which a ray striking the parabolic surface will be totally reflected, n₁, representing the refractive index of air, and n₂ representing the refractive index of said dielectric casing.