OPTICAL DEVICES FOR CONTROLLED COLOR MIXING
First Claim
1. An assembly of multicolor light emitting diodes packaged for controlled color mixing, comprising:
- a substrate;
a plurality of light-emitting diode (LED) dies mounted overlying the substrate, each die emitting light of a corresponding color;
an optically transmissive encapsulant covering the plurality of LED dies; and
at least one lens having a top surface and a bottom surface overlying the encapsulant, the bottom surface of the lens including a predetermined shape to redirect light from each of the plurality of LED dies such that an overlap of the illuminance and luminous intensity distributions of the plurality of LED is substantially increased, wherein the deviation from complete overlap is substantially imperceptible to the average human eye.
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Accused Products
Abstract
The present invention provides a multicolor LED assembly packaged with improved and controlled color mixing to create a more uniform color mixture. The assembly includes at least one lens overlying an encapsulant which encapsulates a plurality of LED dies. The lens includes a top surface and a bottom surface with the contour of the bottom surface designed to redirect light from each of the LED dies in different directions towards the top surface of the lens. The contoured shaped of the bottom surface of the lens redirects light from each of the plurality of LED dies such that illuminance and luminous intensity distributions of the plurality of LED dies substantially overlap, wherein the deviation from complete overlap is less than a predetermined amount which is substantially imperceptible to the average human eye.
150 Citations
63 Claims
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1. An assembly of multicolor light emitting diodes packaged for controlled color mixing, comprising:
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a substrate;
a plurality of light-emitting diode (LED) dies mounted overlying the substrate, each die emitting light of a corresponding color;
an optically transmissive encapsulant covering the plurality of LED dies; and
at least one lens having a top surface and a bottom surface overlying the encapsulant, the bottom surface of the lens including a predetermined shape to redirect light from each of the plurality of LED dies such that an overlap of the illuminance and luminous intensity distributions of the plurality of LED is substantially increased, wherein the deviation from complete overlap is substantially imperceptible to the average human eye. - View Dependent Claims (2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12, 13, 14, 15, 16, 17, 18, 19, 20, 21, 22, 23, 24, 25, 26, 27, 28, 29, 30, 31, 32, 33, 34, 35, 36, 37, 38, 39, 40, 41)
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- 42. A lens for controlled color mixing of a plurality of light-emitting diode (LED) dies, the plurality having at least two colors, said lens having a top surface and a bottom surface overlying the LED dies, the bottom surface of the lens including a predetermined shape to receive and redirect light from each of the plurality of LED dies through and out of the top surface of the lens such that illuminance and luminous intensity distributions of the plurality of LED dies substantially overlap, wherein the deviation from complete overlap is substantially imperceptible to the average human eye.
- 50. A lens for controlled color mixing of a plurality of light-emitting diode (LED) dies, the plurality having at least two colors, said lens overlying the plurality of LED dies and surrounded by a reflector having a spline shape, said lens having at least one surface predetermined to receive and redirect light from each of the plurality of LED dies such that illuminance and luminous intensity distributions of the plurality of LED dies substantially overlap, wherein the deviation from complete overlap is substantially imperceptible to the average human eye.
- 55. A lens for controlled color mixing of a plurality of light-emitting diode (LED) dies, the plurality having at least two colors, said lens overlying the plurality of LED dies and surrounded by an RXI concentrator, said lens having at least one predetermined surface to receive and redirect light from each of the plurality of LED dies such that illuminance and luminous intensity distributions of the plurality of LED dies substantially overlap, wherein the deviation from complete overlap is substantially imperceptible to the average human eye.
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57. A method for determining acceptable color uniformity of a light beam, comprising the steps of:
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choosing three colors at which to make measurements, the each color being a constituent of white light;
for each selected color perform the steps of;
measuring a plurality of x,y chromaticity samples of the light beam, at the selected color, at points in vertical and horizontal distribution extrema where the intensity distribution falls to approximately e−
2 of the on-axis or peak luminous intensity, thereby defining an outer periphery of the light beam;
measuring a plurality of x,y chromaticity samples of the light beam at points located on a spiral from the outer periphery to the on-axis or peak luminous intensity;
measuring a plurality of x,y chromaticity samples of the light beam, for the selected color, at selected angular radials at approximately the full width at half maximum (FWHM) point;
converting mathematically the x,y chromaticity samples for the selected color to a u,v space representation;
plotting MacAdam ellipses from the u,v space representation of the chromaticity samples for the selected color;
calculating a deltaE parameter for the selected color, the deltaE parameter representing the magnitude of the color difference perceived between two color samples which are specified in terms of tristimulus values;
determining acceptable color uniformity for the selected color, wherein acceptable color uniformity for the selected color is attained when the deltaE parameter for the selected color is less than the 2-step MacAdam'"'"'s ellipse or when the deltaE parameter for the selected color matches or exceeds the maximum chromaticity difference of a selected standard;
resulting in acceptable color uniformity of the light beam if the color uniformity for the first color, the second color, and the third color are all acceptable. - View Dependent Claims (58, 59, 60)
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61. A method for using light control facets and randomized facet perturbations of the primary reflector to improve color uniformity, comprising the steps of:
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dividing the primary reflector into horizontal slices and vertical slices, resulting in a plurality of facets, the facets each having a parametric surface described by x=x(φ
, φ
), y=y(φ
, φ
), z=z(φ
, φ
);
calculating transformation vectors a′
=[xφ
, yφ
, zφ
], b′
=[xΨ
, yΨ
, zΨ
] for each facet;
calculating a unit normal vector N′
=(a′
×
b′
)/(sqrt((abs(a′
ˆ
2)abs(b′
ˆ
2)−
abs(a‘
b’
)ˆ
2) for each facet;
calculating a metric tensor, by taking an inner product of a plurality of tangency spaces associated with a reflector facet manifold where the inner product is symmetric, nondegenerate, and bilinear in 3D vector space;
calculating a descriminant g of the metric tensor;
calculating a vector normal to the surface N=r1′
×
r2′
/(sqrt(g))=∈
ij*r′
ˆ
j;
applying a predetermined perturbation to each facet by deviating an angular facet control vector from the unit normal vector by a random angle between an upper and lower bound;
resulting in an integrated primary reflector which both collimates the light, and randomizes color specific phase to improve the intensity distribution function overlap of Cyan, Magenta, and Yellow.
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62. A method to construct an RXI concentrator, comprising the steps of:
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filling the intermediary air of a cassegrain telescope with a refractive dielectric media, the cassegrain telescope comprising a primary reflector and a secondary reflector;
adding a plurality of micro-facets to the primary reflector of the cassegrain telescope;
randomizing the micro-facets with respect to an angle from the normal of each micro-facet using a vector perturbation;
changing the micro-facets into an organic shape or into an arbitrary polygonal parameter shape;
applying the vector perturbation to the secondary reflector using a perturbation factors tessellating the surface of the refractive dielectric at the exit aperture of the RXI concentrator with a plurality of micro-lenslets, each micro-lenslet surface characterized by a sag;
randomizing the sag with one or more of radii, aspherics, NURBS and global Zernike deformation solving the Monge-Ampere partial differential equation, in terms of optimal global deformation on the primary reflector and the secondary reflector;
resulting in an RXI concentrator which optimally combines multi-primary phase in the far field. - View Dependent Claims (63)
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Specification