Optical waveguides

Abstract
An optical waveguide includes a coupling optic and a waveguide body. According to one embodiment, the body includes a first curved surface that extends between an input surface and an end surface and a second surface opposite the first surface. The input surface has a first thickness disposed between the first and second surfaces and the end surface has a second thickness disposed between the first and second surfaces less than the first thickness.
Description
REFERENCE REGARDING FEDERALLY SPONSORED RESEARCH OR DEVELOPMENT

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SEQUENTIAL LISTING

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BACKGROUND OF THE INVENTION

1. Field of the Invention


The present inventive subject matter relates to optical waveguides, and more particularly to optical waveguides for general lighting.


2. Background of the Invention


An optical waveguide mixes and directs light emitted by one or more light sources, such as one or more light emitting diodes (LEDs). A typical optical waveguide includes three main components: one or more coupling elements, one or more distribution elements, and one or more extraction elements. The coupling component(s) direct light into the distribution element(s), and condition the light to interact with the subsequent components. The one or more distribution elements control how light flows through the waveguide and is dependent on the waveguide geometry and material. The extraction element(s) determine how light is removed by controlling where and in what direction the light exits the waveguide.


When designing a coupling optic, the primary considerations are: maximizing the efficiency of light transfer from the source into the waveguide; controlling the location of light injected into the waveguide; and controlling the angular distribution of the light in the coupling optic. One way of controlling the spatial and angular spread of injected light is by fitting each source with a dedicated lens. These lenses can be disposed with an air gap between the lens and the coupling optic, or may be manufactured from the same piece of material that defines the waveguide's distribution element(s). Discrete coupling optics allow numerous advantages such as higher efficiency coupling, controlled overlap of light flux from the sources, and angular control of how the injected light interacts with the remaining elements of the waveguide. Discrete coupling optics use refraction, total internal reflection, and surface or volume scattering to control the distribution of light injected into the waveguide.


After light has been coupled into the waveguide, it must be guided and conditioned to the locations of extraction. The simplest example is a fiber-optic cable, which is designed to transport light from one end of the cable to another with minimal loss in between. To achieve this, fiber optic cables are only gradually curved and sharp bends in the waveguide are avoided. In accordance with well-known principles of total internal reflectance light traveling through a waveguide is reflected back into the waveguide from an outer surface thereof, provided that the incident light does not exceed a critical angle with respect to the surface.


In order for an extraction element to remove light from the waveguide, the light must first contact the feature comprising the element. By appropriately shaping the waveguide surfaces, one can control the flow of light across the extraction feature(s). Specifically, selecting the spacing, shape, and other characteristic(s) of the extraction features affects the appearance of the waveguide, its resulting distribution, and efficiency.


Hulse U.S. Pat. No. 5,812,714 discloses a waveguide bend element configured to change a direction of travel of light from a first direction to a second direction. The waveguide bend element includes a collector element that collects light emitted from a light source and directs the light into an input face of the waveguide bend element. Light entering the bend element is reflected internally along an outer surface and exits the element at an output face. The outer surface comprises beveled angular surfaces or a curved surface oriented such that most of the light entering the bend element is internally reflected until the light reaches the output face


Parker et al. U.S. Pat. No. 5,613,751 discloses a light emitting panel assembly that comprises a transparent light emitting panel having a light input surface, a light transition area, and one or more light sources. Light sources are preferably embedded or bonded in the light transition area to eliminate any air gaps, thus reducing light loss and maximizing the emitted light. The light transition area may include reflective and/or refractive surfaces around and behind each light source to reflect and/or refract and focus the light more efficiently through the light transition area into the light input surface of the light emitting panel. A pattern of light extracting deformities, or any change in the shape or geometry of the panel surface, and/or a coating that causes a portion of the light to be emitted, may be provided on one or both sides of the panel members. A variable pattern of deformities may break up the light rays such that the internal angle of reflection of a portion of the light rays will be great enough to cause the light rays either to be emitted out of the panel or reflected back through the panel and emitted out of the other side.


A.L.P. Lighting Components, Inc. of Niles, Ill., manufactures a waveguide having a wedge shape with a thick end, a narrow end, and two main faces therebetween. Pyramid-shaped extraction features are formed on both main faces. The wedge waveguide is used as an exit sign such that the thick end of the sign is positioned adjacent a ceiling and the narrow end extends downwardly. Light enters the waveguide at the thick end and is directed down and away from the waveguide by the pyramid-shaped extraction features.


SUMMARY OF THE INVENTION

According to one aspect of the present invention, an optical waveguide body includes a first curved surface that extends between an input surface and an end surface and a second surface opposite the first surface. The input surface has a first thickness disposed between the first and second surfaces and the end surface has a second thickness disposed between the first and second surfaces less than the first thickness.


In accordance with another aspect of the present invention, a waveguide body includes a body of optically transmissive material having an input surface for light to enter the body of optically transmissive material along a light path. The body of optically transmissive material is curved and has an inflection region that extends transverse to the light path.


In accordance with yet another aspect of the present invention, a waveguide body comprises a body of optically transmissive material having an input surface for light to enter the body of optically transmissive material along a light path wherein the body of optically transmissive material is curved and has a plurality of inflection regions.


In accordance with a still thither aspect of the present invention, a waveguide includes a body of optically transmissive material. A plurality of LEDs is spaced about the body of optically transmissive material such that light developed by the plurality of LEDs is directed through an input edge surface of the body of optically transmissive surface. Extraction features carried by the body of optically transmissive material are provided for directing light developed by the plurality of LEDs out of the body of optically transmissive material.


In accordance with yet another aspect of the present invention, a coupling optic comprises a coupling optic body including a plurality of input cavities each defined by a wall wherein a projection is disposed in each cavity. Further, a recess is disposed in each projection and the recess of each projection is adapted to receive an associated LED.


Other aspects and advantages of the present invention will become apparent upon consideration of the following detailed description and the attached drawings.





BRIEF DESCRIPTION OF THE DRAWINGS


FIG. 1 is an isometric view of a first embodiment of a waveguide;



FIG. 2 is a side elevational view of the first embodiment of the waveguide;



FIG. 3A is a plan view of the waveguide of FIG. 1;



FIG. 3B is a front elevational view of the waveguide of FIG. 1;



FIG. 4 is a front elevational view of the waveguide body of FIG. 1 shown flattened to illustrate the extraction features;



FIG. 5 is an enlarged fragmentary view of an area 5-5 of FIG. 3;



FIG. 6 is an enlarged fragmentary view of an area 6-6 of FIG. 3;



FIG. 7 is a side isometric view of a second embodiment of a waveguide body having a regular array of extraction features;



FIG. 8 is a sectional view taken generally along the lines 8-8 of FIG. 7;



FIG. 9 is an enlarged, sectional, fragmentary, and isometric view taken along the lines of 9-9 in FIG. 8;



FIG. 1.0 is an enlarged, sectional, fragmentary, and isometric view taken generally along the lines of 10-10 of FIG. 8;



FIG. 11 is an enlarged, fragmentary plan view of several of the extraction features of FIG. 8;



FIG. 12 is an isometric fragmentary view of a third embodiment of a waveguide body having a stepped profile;



FIG. 13 is a plan view of the waveguide body of FIG. 12;



FIG. 14 is a sectional view taken generally along the lines 14-14 of FIG. 13;



FIG. 15 is a fragmentary, enlarged sectional view illustrating the waveguide body of FIGS. 12-14 in greater detail;



FIG. 15A is a view similar to FIG. 15 illustrating an alternative waveguide body;



FIG. 16 is a cross sectional view of a waveguide body having slotted extraction features;



FIG. 16A is a view similar to FIG. 16 showing a segmented slotted extraction feature;



FIGS. 17A-17C are cross sectional views of uncoated, coated, and covered extraction features, respectively;



FIG. 18 is an isometric view of a further embodiment of a waveguide body;



FIG. 19 is plan view of the waveguide body of FIG. 18;



FIG. 20 is a side elevational view of the waveguide body of FIG. 18;



FIG. 21 is a side elevational view of another waveguide body;



FIG. 22 is a plan view of the waveguide body of FIG. 21;



FIG. 23 is a side elevational view of yet another waveguide body;



FIGS. 24-27 are upper isometric, lower isometric, side elevational, and rear elevational views, respectively, of a still further waveguide body;



FIGS. 28-30 are isometric, side elevational, and front elevational views of another waveguide body;



FIGS. 31-46 are isometric views of still further wave ides;



FIG. 44A is a sectional view of the waveguide body of FIG. 44;



FIG. 45A is an isometric view of a hollow waveguide body;



FIGS. 47 and 48 are plan and side views, respectively, of another waveguide body;



FIG. 49 is an enlarged fragmentary view of a portion of the waveguide body of FIG. 48 illustrated by the line 49-49;



FIGS. 50 and 51 are plan and fragmentary sectional views of yet another waveguide body;



FIG. 52 is an isometric view of another waveguide body that is curved in two dimensions;



FIGS. 53-55 are front, bottom, and side elevational views of another waveguide body;



FIG. 56 is an isometric view of alternative extraction features;



FIG. 57 is an isometric view of a waveguide body utilizing at least some of the extraction features of FIG. 56;



FIG. 58 is a fragmentary isometric view of a coupling optic;



FIG. 59 is a fragmentary enlarged isometric view of the coupling optic of FIG. 58;



FIG. 60 is a diagrammatic plan view of another waveguide body;



FIG. 61 is a sectional view taken generally along the lines 61-61 of FIG. 60;



FIG. 62 is a diagrammatic plan view of a still further waveguide body;



FIG. 63 is a sectional view taken generally along the lines 63-63 of FIG. 62;



FIG. 64 is an isometric view of yet another waveguide body;



FIG. 65 is a cross sectional view of the waveguide body of FIG. 64;



FIG. 66 is a cross sectional view of a still further waveguide body;



FIG. 67 is an isometric view of yet another waveguide body having inflection points along the path of light therethrough;



FIG. 68 is a cross sectional view taken generally along the lines 68-68 of FIG. 67; and



FIG. 69 is a side elevational view taken generally along the view lines 69-68 of FIG. 67.





DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

In general, the curvature and/or other shape of a waveguide body and/or the shape, size, and/or spacing of extraction features determine the particular light extraction distribution. All of these options affect the visual uniformity from one end of the waveguide to another. For example, a waveguide body having smooth surfaces may emit light at curved portions thereof. The sharper the curve is, the more light is extracted. The extraction of light along a curve also depends on the thickness of the waveguide body. Light can travel through tight curves of a thin waveguide body without reaching the critical angle, whereas light that travels through a thick waveguide body is more likely to strike the surface at an angle greater than the critical angle and escape.


Tapering a waveguide body causes light to reflect internally along the length of the waveguide body while increasing the angle of incidence. Eventually, this light strikes one side at an angle that is acute enough to escape. The opposite example, i.e., a gradually thickening waveguide body over the length thereof, causes light to collimate along the length with fewer and fewer interactions with the waveguide body walls. These reactions can be used to extract and control light within the waveguide. When combined with dedicated extraction features, tapering allows one to change the incident angular distribution across an array of features. This, in turn, controls how much, and in what direction light is extracted. Thus, a select combination of curves, tapered surfaces, and extraction features can achieve a desired illumination and appearance.


Still further, the waveguide bodies contemplated herein are made of any suitable optically transmissive material, such as an acrylic material, a silicone, a polycarbonate, a glass material, or other suitable material(s) to achieve a desired effect and/or appearance.


As shown in FIGS. 1-3B, a first embodiment of a waveguide 50 comprises a coupling optic 52 attached to a main waveguide body 54. At least one light source 56, such as one or more LEDs, is disposed adjacent to the coupling optic 52. The light source 56 may be a white LED or may comprise multiple LEDs including a phosphor-coated LED either alone or in combination with a color LED, such as a green LED, etc. In those cases where a soft white illumination is to be produced, the light source 56 typically includes a blue shifted yellow LED and a red LED. Different color temperatures and appearances could be produced using other LED combinations, as is known in the art. In one embodiment, the light source 56 comprises any LED, for example, an MT-G LED incorporating TrueWhite® LED technology as developed and manufactured by Cree, Inc., the assignee of the present application.


The waveguide body 54 has a curved, tapered shape formed by a first surface 58 and a second surface 60. Light emitted from the light source 56 exits an output surface 62 of the coupling optic 52 and enters an input surface 64 at a first end 66 of the waveguide body 54. Light is emitted through the first surface 58 and reflected internally along the second surface 60 throughout the length of the waveguide body 54. The waveguide body 54 is designed to emit all or substantially all of the light from the first surface 58 as the light travels through the waveguide body 54. Any remaining light may exit the waveguide 54 at an end surface 70 located at a second end 68 opposite the first end 66. Alternatively, the end surface 70 may be coated with a reflective material, such as a white or silvered material to reflect any remaining light back into the waveguide body 54, if desired.


The curvature of the first surface 58 of the waveguide body 54 allows light to escape, whereas the curvature of the second surface 60 of the waveguide body 54 prevents the escape of light through total internal reflection. Specifically, total internal reflection refers to the internal reflection of light within the waveguide body that occurs when the angle of incidence of the light ray at the surface is less than a threshold referred to as the critical angle. The critical angle depends on the indices of refraction (N) of the material of which the waveguide body is composed and of the material adjacent to the waveguide body. For example, if the waveguide body is an acrylic material having an index of refraction of approximately 1.5 and is surrounded by air, the critical angle, θc, is as follows:

θc=arcsin(Nacrylic/Nair)=arcsin(1.5/1)=41.8°


In the first embodiment, light is emitted through the first surface 58 of the waveguide body 54 in part due to the curvature thereof.


As shown in FIGS. 1 and 2, the taper of the waveguide body 54 is linear between the input surface 64 and the end surface 70. According to one embodiment, a first thickness at the input surface 64 is 6 mm and a second thickness of the end surface is 2 mm. The radius of curvature of the first surface 58 is approximately 200 mm and the radius of the curvature of the second surface 60 is approximately 200 mm.


Further, the number, geometry, and spatial array of optional extraction features across a waveguide body affects the uniformity and distribution of emitted light. As shown in the first embodiment of the waveguide body 54 in FIGS. 3A, 3B and 4-6, an array of discrete extraction features 72 having a variable extraction feature size is utilized to obtain a uniform or nearly uniform distribution of light. Specifically, the extraction features 72 are arranged in rows and columns Wherein the features in each row extend left to right and the features in each column extend top to bottom as seen in FIGS. 3A and 3B. The extraction features 72 closest to the light source may be generally smaller and/or more widely spaced apart so that in the length dimension of the waveguide body 54 the majority of light travels past such features to be extracted at subsequent parts of the waveguide body 54. This results in a gradual extraction of light over the length of the waveguide body 54. The center-to-center spacing of extraction features 72 in each row are preferably constant, although such spacing may be variable, if desired. The extraction features 72 contemplated herein may be formed by injection molding, embossing, laser cutting, calender rolling, or the extraction features may added to the waveguide body 54 by a film.


Referring to FIGS. 3A and 3B, extraction features 72 on the first surface 58 of the waveguide body 54 permit the light rays to exit the waveguide body 54 because the angles of incidence of light rays at the surface of the extraction features 72 are greater than the critical angle. The change in size (and, optionally, spacing) of the extraction features 72 over the length of the waveguide body 54 results in a uniform or nearly uniform distribution of light emitted from the waveguide body 54 over the length and width thereof. Preferably, as seen in FIGS. 4 and 5, the extraction features 72 nearest the light source 56 are approximately 0.5 mm in width by 0.5 mm in length and 0.5 mm in depth. Also preferably, the extraction features at such location have a center-to-center spacing of about 2 mm. Still thither, as seen in FIGS. 4 and 6, the extraction features 72 farthest from the light source 56 are preferably approximately 1.4 mm (width) by 1.4 mm (length) by 1.4 mm (depth). In addition, the extraction features 72 at such location are also spaced apart about 2 mm (measured center-to-center). While the extraction features 72 are illustrated as having a constant spacing along the waveguide body 54, the features may instead have variable spacing as noted above. Thus, for example, the spacing between the features may decrease with distance from the light source 56. The increased size (and, possibly, density) of extraction features 72 as seen in FIG. 6 allows for the same amount of light to be emitted as the smaller extraction features 72 seen in FIG. 5. While a uniform distribution of light is desired in the first embodiment, other distributions of light may be contemplated and obtained using different arrays of extraction features.


Referring next to FIGS. 7-11, a further embodiment of a waveguide body 74 is illustrated. The waveguide body 74 is identical to the waveguide body 54, with the exception that the sizes and densities of extraction features 76 are constant along an outer surface 77. The waveguide body 74 further includes an input surface 78, an end surface 79 opposite the input surface 78, and an inner surface 80 and is adapted to be used in conjunction with any coupling optic and one or more light sources, such as the coupling optics disclosed herein and the LED 56 of the previous embodiment. The dimensions and shape of the waveguide body 74 are identical to those of the previous embodiment.


As seen in FIGS. 9-11, each extraction feature 76 comprises a V-shaped notch formed by flat surfaces 81, 82, End surfaces 83, 84 are disposed at opposing ends of the surfaces 81, 82. The end surfaces 83, 84 are preferably, although not necessarily, substantially normal to the surface 77. In one embodiment, as seen in FIG. 9, the surface 81 is disposed at an angle a1 with respect to the surface 77 whereas the surface 82 is disposed at an angle a2 with respect to the surface 77. While the angles a1 and a2 are shown as being equal or substantially equal to one another in FIGS. 9-11, the objective in a preferred embodiment is to extract all or substantially all light during a single pass through the waveguide body from the input surface 78 to the end surface 79. Therefore, light strikes only the surfaces 81, and little to no light strikes the surfaces 82. In such an embodiment the surfaces 81, 82 are be disposed at different angles with respect to the surface 77, such that a1 is about equal to 140 degrees and a2 is about equal to 95 degrees, as seen in FIG. 17A.


The extraction features 76 shown in FIGS. 9-11 may be used as the extraction features 72 of the first embodiment, it being understood that the size and spacing of the extraction features may vary over the surface 58, as noted previously. The same or different extraction features could be used in any of the embodiments disclosed herein as noted in greater detail hereinafter, either alone or in combination.


Referring to FIGS. 12-15, a third embodiment of a waveguide body 90 utilizes extraction features 92 in the form of a plurality of discrete steps 94 on a surface 98 of the waveguide body 90. The waveguide body 90 has an input surface 91 and an end surface 93. The steps 94 extend from side to side of the waveguide body 90 whereby the input surface 91 has a thickness greater than the thickness of the end surface 93. Any coupling optic, such as any of the coupling optics disclosed herein, may be used with the waveguide body 90, Light either refracts or internally reflects via total internal reflection at each of the steps 94. The waveguide body 90 may be flat (i.e., substantially planar) or curved in any shape, smooth or textured, and/or have a secondary optically refractive or reflective coating applied thereon. Each step 94 may also be angled, for example, as shown by the tapered surfaces 96 in FIG. 15, although the surfaces 96 can be normal to adjacent surfaces 98, if desired.



FIG. 15A illustrates an embodiment wherein extraction features 92 include surfaces 96 that form an acute angle with respect to adjacent surfaces 98, contrary to the embodiment of FIG. 15. In this embodiment, the light rays traveling from left to right as seen in FIG. 15A are extracted out of the surface including the surfaces 96, 98 as seen in FIG. 15, as opposed to the lower surface 99 (seen in FIGS. 14 and 15).


Yet another modification of the embodiment of FIGS. 12-15 is seen in FIGS. 47-49 wherein the tapered waveguide body 90 includes extraction features 92 having surfaces 96 separated from one another by intermediate step surfaces 95. The waveguide body 90 tapers from a first thickness at the input surface 91 to a second, lesser thickness at the end surface 93. Light is directed out of the lower surface 99.


Further, the steps 94 may be used in conjunction with extraction features 76 that are disposed in the surfaces 98 or even in each step 94. This combination allows for an array of equally spaced extraction features 72 to effect a uniform distribution of light. The changes in thickness allows for a distribution of emitted light without affecting the surface appearance of the waveguide.


Extraction features may also be used to internally reflect and prevent the uncontrolled escape of light. For example, as seen in FIG. 17A, a portion of light that contacts a surface 81 of a typical extraction feature 76 escapes uncontrolled. FIG. 16 illustrates a waveguide body 108 having a slotted extraction feature 110 that redirects at least a portion of light that would normally escape back into the waveguide body 108. The slotted extraction feature 110 comprises a parallel-sided slot having a first side surface 111 and a second side surface 112. A portion of the light strikes the slotted extraction feature 110 at a sufficiently high angle of incidence that the light escapes through the first side surface 111. However, most of the escaped light reenters the waveguide body 108 through the second side surface 112. The light thereafter reflects off the outer surface of the waveguide body 108 and remains inside the body 108. The surface finish and geometry of the slotted extraction feature 110 affect the amount of light that is redirected back into the waveguide body 108. If desired, a slotted extraction feature 110 may be provided in upper and lower surfaces of the waveguide body 108. Also, while a flat slot is illustrated in FIG. 16, curved or segmented slots are also possible. For example, FIG. 16A illustrates a curved and segmented slot comprising slot portions 114a, 114b. Parallel slotted extraction features may be formed within the waveguide as well as at the surface thereof, for example, as seen at 113 in FIG. 16. Any of the extraction features disclosed herein may be used in or on any of the waveguide bodies disclosed herein. The extraction features may be equally or unequally sized, shaped, and/or spaced in and/or on the waveguide body.


In addition to the extraction features 72, 76, 94, 110, 113, and/or 114, light may be controlled through the use of discrete specular reflection. An extraction feature intended to reflect light via total internal reflection is limited in that any light that strikes the surface at an angle greater than the critical angle will escape uncontrolled rather than be reflected internally. Specular reflection is not so limited, although specular reflection can lead to losses due to absorption. The interaction of light rays and extraction features 102 with and without a specular reflective surface is shown in FIGS. 17A-17C. FIG. 17A shows the typical extraction feature 76 with no reflective surface. FIG. 17B shows a typical extraction feature 76 with a discrete reflective surface 115 formed directly thereon. The discrete reflective surface 115 formed on each extraction feature 76 directs any light that would normally escape through the extraction feature 76 back into the waveguide body 74. FIG. 17C shows an extraction feature 76 with a discrete reflective surface 116 having an air gap 117 therebetween. In this embodiment, light either reflects off the surface 81 back into the waveguide body 74 or refracts out of the surface 81. The light that does refract is redirected back into the waveguide body 74 by the reflective surface 116 after traveling through the air gap 117. The use of non-continuous reflective surfaces localized at points of extraction reduces the cost of the reflective material, and therefore, the overall cost of the waveguide. Specular reflective surfaces can be manufactured by deposition, bonding, co-extrusion with extraction features, insert molding, vacuum metallization, or the like.


Referring to FIGS. 18-20, a further embodiment of a waveguide body 120 includes a curved, tapered shape formed by a first surface 122 and a second surface 124. Similar to the first embodiment of the waveguide 54, light enters an input surface 126 at a first end 128 of the waveguide 120. Light is emitted through the first surface 122 and reflected internally along the second surface 124 throughout the length of the waveguide body 120. The waveguide body 120 is designed to emit all or substantially all of the light from the first surface 122 as the light travels through the waveguide body 120. Thus, little or no light is emitted out an end face 132 opposite the first end 128.



FIG. 20 shows a cross-section of the waveguide 120 body taken along the width thereof. The distance 134 between the first and second surfaces 122, 124 is constant along the width. The first and second surfaces 122, 124 have a varied contour that comprises linear portions 136 and curved portions 138. The waveguide body 120 has a plurality of extraction features 140 that are equally or unequally spaced on the surface 122 and/or which are of the same or different size(s) and/or shape(s), as desired. As noted in greater detail hereinafter, the embodiment of FIGS. 18-20 has multiple inflection regions that extend transverse to the general path of light through the input surface 126. Further, as in all the embodiments disclosed herein, that waveguide body is made of an acrylic material, a silicone, a polycarbonate, a glass material, or the like.



FIGS. 21 and 22 illustrate yet another embodiment wherein a series of parallel, equally-sized linear extraction features 198 are disposed in a surface 199 at varying distances between an input surface 200 of a waveguide body 202. Each of the extraction features 198 may be V-shaped and elongate such that extraction features 198 extend from side to side of the waveguide body 202. The spacing between the extraction features 198 decreases with distance from the input surface 200 such that the extraction features are closest together adjacent an end surface 204. The light is extracted out of a surface 206 opposite the surface 199.



FIG. 23 illustrates an embodiment identical to FIGS. 21 and 22, with the exception that the waveguide features 198 are equally spaced and become larger with distance from the input face 200. If desired, the extraction features 198 may be unequally spaced between the input and end surfaces 200, 204, if desired. As in the embodiment of FIGS. 21 and 22, light is extracted out of the surface 206.



FIGS. 24-27 illustrate yet another embodiment of a waveguide body 240 having an input surface 242, an end surface 244, and a J-shaped body 246 disposed between the surfaces 242, 244. The waveguide body 240 may be of constant thickness as seen in FIGS. 24-27, or may have a tapering thickness such that the input surface 242 is thicker than the end surface 244. Further, the embodiment of FIGS. 24-27 is preferably of constant thickness across the width of the body 240, although the thickness could vary along the width, if desired. One or more extraction features may be provided on an outer surface 248 and or an inner surface 250, if desired, although it should be noted that light injected into the waveguide body 240 escapes the body 240 through the surface 248 due to the curvature thereof.



FIGS. 28-30 illustrate a still further embodiment of a waveguide 260 including an input surface 262. The waveguide body 260 further includes first and second parallel surfaces 264, 266 and beveled surfaces 268, 270 that meet at a line 272. Light entering the input surface 262 escapes through the surfaces 268, 270.


A further embodiment comprises the curved waveguide body 274 of FIG. 31. Light entering an input surface 275 travels through the waveguide body 274 and is directed out an outer surface 276 that is opposite an inner surface 277. As in any of the embodiments disclosed herein, the surfaces 276, 277 may be completely smooth, and/or may include one or more extraction features as disclosed herein. Further, the waveguide body may have a constant thickness (i.e. the dimension between the faces 276, 277) throughout, or may have a tapered thickness between the input surface 275 and an end surface 278, as desired. As should be evident from an inspection of FIG. 31, the waveguide body 274 is not only curved in one plane, but also is tapered inwardly from top to bottom (i.e., transverse to the plane of the curve of the body 274) as seen in the FIG.


In the case of an arc of constant radius, a large portion of light is extracted at the beginning of the arc, while the remaining light skips along the outside surface. If the bend becomes sharper with distance along the waveguide body, a portion of light is extracted as light skips along the outside surface. By constantly spiraling the arc inwards, light can be extracted out of the outer face of the arc evenly along the curve. Such an embodiment is shown by the spiral-shaped waveguide body 280 of FIG. 32 (an arrow 282 illustrates the general direction of light entering the waveguide body 280 and the embodiments shown in the other FIGS.). These same principles apply to S-bends and arcs that curve in two directions, like a corkscrew. For example, an S-shaped waveguide body 290 is shown in FIG. 33 and a corkscrew-shaped waveguide body 300 is shown in FIG. 34. Either or both of the waveguide bodies is of constant cross sectional thickness from an input surface to an end surface or is tapered between such surfaces. The surfaces may be smooth and/or may include extraction features as disclosed herein. The benefit of these shapes is that they produce new geometry to work with, new ways to create a light distribution, and new ways to affect the interaction between the waveguide shape and any extraction features.



FIGS. 35-46 illustrate further embodiments of waveguide bodies 310, 320, 330, 340, 350, 360, 370, 380, 390, 400, and 410, respectively, wherein curvature, changes in profile and/or cross sectional shape and thickness are altered to create a number of effects. The waveguide body 310 is preferably, although not necessarily, rectangular in cross sectional shape and has a curved surface 312 opposite a flat surface 314. The curved surface 312 has multiple inflection regions defining a convex surface 312a and a convex surface 312b. Both of the surfaces 312, 314 may be smooth and/or may have extraction features 316 disposed therein (as may all of the surfaces of the embodiments disclosed herein.) Referring to FIGS. 36 and 37, the waveguide bodies 320, 330 preferably, although not necessarily, have a rectangular cross sectional shape, and may include two sections 322, 324 (FIG. 36) or three or more sections 332, 334, 336 (FIG. 37) that are disposed at angles with respect to one another. FIG. 38 illustrates the waveguide body 340 having a base portion 342 and three curved sections 344a-344c extending away from the base portion 342. The cross sections of the base portion 342 and the curved portions 344 are preferably, although not necessarily, rectangular in shape.



FIGS. 39 and 40 illustrate waveguide bodies 350 and 360 that include base portions 352, 362, respectively. The waveguide body 350 of FIG. 39 includes diverging sections 354a, 354b having outer surfaces 356a, 356b extending away from the base portion 352 that curve outwardly in convex fashion. The waveguide body 360 of FIG. 40 includes diverging sections 364a, 364b having outer surfaces 366a, 366b that curve outwardly in convex and concave fashion.


The waveguide bodies 370, 380, and 390 of FIGS. 41-43 all have circular or elliptical cross sectional shapes. The waveguide bodies 370, 380 have two sections 372, 374 (FIG. 41) or three or more sections 382, 384, 386 (FIG. 42). The waveguide body 390 of FIG. 43 preferably, although not necessarily, has a circular or elliptical cross sectional shape and, like any of the waveguide bodies disclosed herein (or any section or portion of any of the waveguide bodies disclosed herein) tapers from an input surface 392 to an output surface 394.


The waveguide body 400 of FIGS. 44 and 44A is substantially mushroom-shaped in cross section comprising a base section 402 that may be circular in cross section and a circular cap section 404. Extraction features 406 may be provided in the cap section 404. Light may be emitted from a cap surface 408.



FIGS. 45 and 46 illustrate that the cross sectional shape may be further varied, as desired. Thus, for example, the cross sectional shape may be triangular as illustrated by the waveguide body 410 or any other shape. If desired, any of the waveguide bodies may be hollow, as illustrated by the waveguide body 412 seen in FIG. 45A, which is identical to the waveguide body 410 of FIG. 45 except that a triangular recess 414 extends fully therethrough. FIG. 46 illustrates substantially sinusoidal outer surfaces 422, 424 defining a complex cross sectional shape.



FIG. 50 illustrates a waveguide body 440 that is preferably, although not necessarily, planar and of constant thickness throughout. Light is directed into opposing input surfaces 442a, 442h and transversely through the body 440 by first and second light sources 56a, 56b, each comprising, for example, one or more LEDs, and coupling optics 52a, 52b, respectively, which together form a waveguide. Extraction features 444, which may be similar or identical to the extraction features 76 or any of the other extraction features disclosed herein, are disposed in a surface 446. As seen in FIG. 51 light developed by the light sources 56a, 56b is directed out a surface 448 opposite the surface 446. As seen in FIG. 50, the density and/or sizes of the extraction features 444 are relatively low at areas near the input surfaces 442a, 442b and the density and/or sizes are relatively great at an intermediate area 450. Alternatively, or in addition, the shapes of the extraction features may vary over the surface 446. A desired light distribution, such as a uniform light distribution, is thus obtained.


As in other embodiments, extraction features may be disposed at other locations, such as in the surface 448, as desired.



FIG. 52 illustrates a waveguide body 460 that is curved in two dimensions. Specifically, the body 460 is curved not only along the length between an input surface 462 and an end surface 464, but also along the width between side surfaces 466, 468. Preferably, although not necessarily, the waveguide body is also tapered between the input surface 462 and the end surface 464, and is illustrated as having smooth surfaces, although one or more extraction features may be provided on either or both of opposed surfaces 470, 472.



FIGS. 53-55 illustrate a waveguide body 490 that is also curved in multiple dimensions. An input surface 492 is disposed at a first end and light is transmitted into first and second (or more) sections 493, 494. Each section 493, 494 is tapered and is curved along the length and width thereof. Light is directed out of the waveguide body 490 downwardly as seen in FIG. 53.



FIG. 56 illustrates various alternative extraction feature shapes. Specifically, extraction features 550, 552 comprise convex and concave rounded features, respectively. Extraction features 554, 556 comprise outwardly extending and inwardly extending triangular shapes, respectively (the extraction feature 556 is similar or identical to the extraction feature 76 described above). Extraction features 558, 560 comprise outwardly extending and inwardly extending inverted triangular shapes, respectively. FIG. 57 shows a waveguide body 570 including any or all of the extraction features 550-560. The sizes and/or density of the features may be constant or variable, as desired.


Alternatively or in addition, the extraction features may have any of the shapes of copending U.S. patent application Ser. No. 13/840,563, entitled “Optical Waveguide and Lamp Including Same”, owned by the assignee of the present application and filed contemporaneously with the present application, the disclosure of which is expressly incorporated by reference herein.


If desired, one or more extraction features may extend fully through any of the waveguide bodies described herein, for example, as seen in FIG. 17D. Specifically, the extraction feature 76 may have a limited lateral extent (so that the physical integrity of the waveguide body is not impaired) and further may extend fully through the waveguide body 74. Such an extraction feature may be particularly useful at or near an end surface of any of the waveguide bodies disclosed herein.


Referring next to FIGS. 60 and 61, a further embodiment comprises a waveguide body 580 and a plurality of light sources that may comprise LEDs 582a-582d. While four LEDs are shown, any number of LEDs may be used instead. The LEDs 582 direct light radially into the waveguide body 580. In the illustrated embodiment, the waveguide body 580 is circular, but the body 580 could be any other shape, for example as described herein, such as square, rectangular, curved, etc. As seen in FIG. 61, and as in previous embodiments, the waveguide body 580 includes one or more extraction features 583 arranged in concentric and coaxial sections 583a-583d about the LEDs to assist in light extraction. The extraction features are similar or identical to the extraction features of copending U.S. patent application Ser. No. 13/840,563, entitled “Optical Waveguide and Lamp Including Same”, incorporated by reference herein. Light extraction can occur out of one or both of opposed surfaces 584, 586. Still further, the surface 586 could be tapered and the surface 584 could be flat, or both surfaces 584, 586 may be tapered or have another shape, as desired.



FIGS. 62 and 63 illustrate yet another waveguide body 590 and a plurality of light sources that may comprise LEDs 592a-592d. While four LEDs 592 are shown, any number of LEDs may be used instead. In the illustrated embodiment, the waveguide body 590 is circular in shape, but may be any other shape, including the shapes disclosed herein. The light developed by the LEDs is directed axially downward as seen in FIG. 63. The downwardly directed light is diverted by a beveled surface 594 of the waveguide body 590 radially inwardly by total internal reflection. The waveguide body 590 includes one or more extraction features 595 similar or identical to the extraction features of FIGS. 60 and 61 arranged in concentric and coaxial sections 595a-595d relative to the LEDs 592a-592d, also as in the embodiment of FIGS. 62 and 63, Light is directed by the extraction features 595 out one or both opposed surfaces 596, 598. If desired, the surface 598 may be tapered along with the surface 596 and/or the surface 596 may be flat, as desired.


A still further embodiment of a waveguide body 600 is shown in FIGS. 64 and 65. The body 600 has a base portion 602 and an outwardly flared main light emitting portion 604. The base portion may have an optional interior coupling cavity 606 comprising a blind bore within which is disposed one or more light sources in the form of one or more LEDs 610 (FIG. 65). If desired, the interior coupling cavity 606 may be omitted and light developed by the LEDs 610 may be directed through an air gap into a planar or otherwise shaped input surface 614. The waveguide body 600 is made of any suitable optically transmissive material, as in the preceding embodiments. Light developed by the LED's travels through the main light emitting portion 604 and out an inner curved surface 616.



FIG. 66 illustrates an embodiment identical to FIGS. 64 and 65 except that the interior coupling cavity comprises a bore 617 that extends fully through the base portion 602 and the one or more light sources comprising one or more LEDs 610 extend into the bore 617 from an inner end as opposed to the outside end shown in FIGS. 64 and 65. In addition, a light diverter comprising a highly reflective conical plug member 618 is disposed in the outside end of the bore 617. The plug member 618 may include a base flange 619 that is secured by any suitable means, such as an adhesive, to an outer surface of the waveguide body 600 such that a conical portion 620 extends into the bore 617. If desired, the base flange 619 may be omitted and the outer diameter of the plug member 618 may be slightly greater than the diameter of the bore 617 whereupon the plug member 618 may be press fitted or friction fitted into the bore 617 and/or secured by adhesive or other means. Still further, if desired, the conical plug member 618 may be integral with the waveguide body 600 rather than being separate therefrom. Further, the one or more LEDs 610 may be integral with the waveguide body 600, if desired. In the illustrated embodiment, the plug member 618 may be made of white polycarbonate or any other suitable material, such as acrylic, molded silicone, polytetrafluoroethylene (PTFE), or Delrin® acetyl resin. The material may be coated with reflective silver or other metal or material using any suitable application methodology, such as a vapor deposition process.


Light developed by the one or more LEDs is incident on the conical portion 620 and is diverted transversely through the base portion 602. The light then travels through the main light emitting portion 604 and out the inner curved surface 616. Additional detail regarding light transmission and extraction is provided in copending U.S. patent application Ser. No. 13/840,563, entitled “Optical Waveguide and Lamp Including Same”, incorporated by reference herein.


In either of the embodiments shown in FIGS. 64-66 additional extraction features as disclosed herein may be disposed on any or all of the surfaces of the waveguide body 600.


Other shapes of waveguide bodies and extraction features are possible. Combining these shapes stacks their effects and changes the waveguide body light distribution further. In general, the waveguide body shapes disclosed herein may include one or multiple inflection points or regions where a radius of curvature of a surface changes either abruptly or gradually. In the case of a waveguide body having multiple inflection regions, the inflection regions may be transverse to the path of light through the waveguide body (e.g., as seen in FIGS. 18-20), along the path of light through the waveguide body (e.g., shown in FIG. 33), or both (e.g., as shown by the waveguide body 640 of FIGS. 67-69 or by combining waveguide bodies having both inflection regions). Also, successive inflection regions may reverse between positive and negative directions (e.g., there may be a transition between convex and concave surfaces), Single inflection regions and various combinations of multiple inflection regions, where the inflection regions are along or transverse to the path of light through the waveguide body or multiple waveguide bodies are contemplated by the present invention.


Referring again to FIGS. 1 and 3A, light developed by the one or more LEDs 56 is transmitted through the coupling optic 52. If desired, an air gap is disposed between the LED(s) 56 and the coupling optic 52. Any suitable apparatus may be provided to mount the light source 56 in desired relationship to the coupling optic 52. The coupling optic 52 mixes the light as close to the light source 56 as possible to increase efficiency, and controls the light distribution from the light source 56 into the waveguide body. When using a curved waveguide body as described above, the coupling optic 52 can control the angle at which the light rays strike the curved surface(s), which results in controlled internal reflection or extraction at the curved surface(s).


If desired, light may be alternatively or additionally transmitted into the coupling optic 52 by a specular reflector at least partially or completely surrounding each or all of the LEDs.


As seen in FIGS. 58 and 59, a further embodiment of a coupling optic 600 having a coupling optic body 601 is shown. The coupling optic is adapted for use with at least one, and preferably a plurality of LEDs of any suitable type. The coupling optic body 601 includes a plurality of input cavities 602a, 602b, . . . , 602N each associated with and receiving light from a plurality of LEDs (not shown in FIGS. 58 and 59, but which are identical or similar to the LED 56 of FIG. 1). The input cavities 602 are identical to one another and are disposed in a line adjacent one another across a width of the coupling optic 600. As seen in FIG. 59, each input cavity 602, for example, the input cavity 602h, includes an approximately racetrack-shaped wall 606 surrounded by arcuate upper and lower marginal surfaces 608a, 608b, respectively. A curved surface 610 tapers between the upper marginal surface 608a and a planar upper surface 612 of the coupling optic 600. A further curved surface identical to the curved surface 610 tapers between the lower marginal surface 608b and a planar lower surface of the coupling optic 600.


A central projection 614 is disposed in a recess 616 defined by the wall 606. The central projection 614 is, in turn, defined by curved wall sections 617a-617d. A further approximately racetrack-shaped wall 618 is disposed in a central portion of the projection 614 and terminates at a base surface 620 to form a further recess 622. The LED associated with the input cavity 602b in mounted by any suitable means relative to the input cavity 602b so that the LED extends into the further recess 622 with an air gap between the LED and the base surface 620. The LED is arranged such that light emitted by the LED is directed into the coupling optic 600. If desired, a reflector (not shown) may be disposed behind and/or around the LED to increase coupling efficiency. Further, any of the surfaces may be coated or otherwise formed with a reflective surface, as desired.


In embodiments such as that shown in FIGS. 58 and 59 where more than one LED is connected to a waveguide body, the coupling optic 600 may reduce the dead zones between the light cones of the LEDs. The coupling optic 600 may also control how the light cones overlap, which is particularly important when using different colored LEDs. Light mixing is advantageously accomplished so that the appearance of point sources is minimized.


As shown in FIGS. 1 and 12, the coupling optic guide 52 introduces light emitted from the light source 56 to the waveguide 54. The light source 56 is disposed adjacent to a coupling optic 82 that has a cone shape to direct the light through the coupling optic guide 52. The coupling optic 82 is positioned within the coupling optic guide 52 against a curved indentation 84 formed on a front face 86 opposite the output face 62 of the coupling optic guide 52. The light source 56 is positioned outside of the coupling optic guide 52 within the curved indentation 84. An air gap 85 between the light source 56 and the indentation 84 allows for mixing of the light before the light enters the coupling optic 82. Two angled side surfaces 88, the front face 86, and the output face 62 may be made of a plastic material and are coated with a reflective material. The coupling optic guide 52 is hollow and filled with air.


Other embodiments of the disclosure including all of the possible different and various combinations of the individual features of each of the foregoing embodiments and examples are specifically included herein.


INDUSTRIAL APPLICABILITY

The waveguide components described herein may be used singly or in combination. Specifically, a flat, curved, or otherwise-shaped waveguide body with or without discrete extraction features could be combined with any of the coupling optics and light sources described herein. In any case, one may obtain a desired light output distribution.


Numerous modifications to the present disclosure will be apparent to those skilled in the art in view of the foregoing description. Accordingly, this description is to be construed as illustrative only and is presented for the purposes of enabling those skilled in the art to make and use the present disclosure and to teach the best mode of carrying out the same.

Claims
  • 1. An optical waveguide body, comprising: a first surface that extends between an input surface and an end surface;a second surface opposite the first surface wherein a body thickness is disposed between the first and second surfaces;wherein the body thickness at the input surface is greater than the body thickness at the end surface and the body thickness between the input surface and end surface decreases over a length of the body;and at least one stepped feature defined by first and second oblique angles on one of the first and second surface;wherein the first surface is curved along an entire first extent between the input surface and the end surface, and wherein the first surface is curved along an entire second extent between side surfaces wherein the first extent is orthogonal to the second extent.
  • 2. The optical waveguide body of claim 1, wherein light is emitted through the first surface.
  • 3. The optical waveguide body of claim 2, wherein light is internally reflected along the first and second surfaces.
  • 4. The optical waveguide body of claim 1, wherein the first thickness is approximately 6 mm, the second thickness is approximately 2 mm, and the first surface comprises a radius of curvature of approximately 200 mm.
  • 5. The optical waveguide body of claim 1, wherein the waveguide comprises a length between the input surface and the end surface and a width transverse to the length, wherein a distance between the first surface and the second surface decreases at least a portion along the width, and wherein the second surface is curved.
  • 6. The optical waveguide body of claim 1, further comprising at least one extraction feature.
  • 7. The optical waveguide body of claim 6, wherein the at least one extraction feature is located within the body.
  • 8. The optical waveguide body of claim 6, wherein the at least one extraction feature is located on an outer surface of the body.
  • 9. The optical waveguide body of claim 6, wherein the at least one extraction feature is an angled slot comprising parallel sides.
  • 10. The optical waveguide body of claim 6, further comprising a reflective surface.
  • 11. The optical waveguide body of claim 10, wherein the reflective surface is disposed adjacent to the at least one extraction feature.
  • 12. The optical waveguide body of claim 6, wherein the extraction feature comprises a stepped feature.
  • 13. The optical waveguide body of claim 12, wherein the stepped feature is formed on the first surface.
  • 14. The optical waveguide body of claim 1, further comprising an array of extraction features on the first surface.
  • 15. The optical waveguide body of claim 14, wherein the extraction features comprise sizes that vary across the first surface.
  • 16. The optical waveguide body of claim 14, further comprising at least one reflective surface adjacent to at least one extraction feature.
  • 17. The optical waveguide body of claim 1, in combination with a coupling optic.
  • 18. The optical waveguide body of claim 1, further in combination with a light source.
  • 19. The optical waveguide body of claim 1, further including unequally spaced extraction features disposed on the first surface.
  • 20. The optical waveguide body of claim 1, further including unequally sized extraction features disposed on the first surface.
  • 21. The optical waveguide body of claim 1, further including unequally shaped extraction features disposed on the first surface.
  • 22. The optical waveguide body of claim 1, further including equally spaced extraction features disposed on the first surface.
  • 23. The optical waveguide body of claim 1, further including equally sized extraction features disposed on the first surface.
  • 24. The optical waveguide body of claim 1, further including equally shaped extraction features disposed on the first surface.
  • 25. The optical waveguide body of claim 1, wherein the body is made of a material selected from the group comprising an acrylic material, a silicone, a polycarbonate, and a glass material.
  • 26. An optical waveguide body, comprising: a first surface that extends between an input surface and an end surface;a second surface opposite the first surface;wherein the input surface comprises a first thickness disposed between the first and second surfaces;wherein the end surface comprises a second thickness disposed between the first and second surfaces less than the first thickness;wherein at least one of the first and second surfaces comprises first and second pluralities of spaced surfaces wherein each surface of the first plurality of spaced surfaces is disposed between and comprises ends coincident with ends of successive surfaces of the second plurality of spaced surfaces and the first and second pluralities of spaced surfaces define an overall body thickness that does not increase at any point from the input surface to the end surface;wherein the waveguide body develops a light distribution for general lighting;wherein at least one of the surfaces of the first and second pluralities of spaced surfaces is disposed at an oblique angle with respect to an adjacent other surface of the first and second pluralities of spaced surfaces; andwherein the first and the second pluralities of spaced surfaces are unequally spaced.
  • 27. The optical waveguide body of claim 26, wherein at least one of the surfaces of the first and second pluralities is disposed at an obtuse angle with respect to an adjacent other surface of the first and second pluralities.
  • 28. The optical waveguide body of claim 26, wherein at least one of the surfaces of the first and second pluralities is disposed at an acute angle with respect to an adjacent other surface of the first and second pluralities.
  • 29. The optical waveguide body of claim 26, wherein an optical feature is disposed on at least one of the surfaces of the first and second pluralities.
  • 30. The optical waveguide body of claim 29, wherein the optical feature is an extraction feature.
  • 31. The optical waveguide body of claim 26, wherein the overall body thickness decreases between the input surface and the end surface.
  • 32. The optical waveguide body of claim 31, wherein the overall body thickness decreases with at least one of the first and second pluralities of surfaces.
  • 33. An optical waveguide body, comprising: a first surface extending in a length dimension between an input surface and an end surface and the first surface extending in a width dimension orthogonal to the length dimension;a second surface opposite the first surface;wherein the input surface comprises a first thickness disposed between the first and second surfaces;wherein the end surface comprises a second thickness disposed between the first and second surfaces less than the first thickness; andwherein at least one stepped feature is located on one of the first and second surfaces and a plurality of discrete optical features is disposed on the at least one stepped feature and the discrete optical features are disposed in a sequence extending along the width dimension.
  • 34. The optical waveguide body of claim 33, wherein the at least one stepped feature is defined by first and second obtuse angles on one of the first and second surfaces.
  • 35. The optical waveguide body of claim 33, wherein the at least one stepped feature is defined by at least one acute angle on one of the first and second surfaces.
  • 36. The optical waveguide body of claim 33, wherein the at least one stepped feature is defined by at least one obtuse angle on one of the first and second surfaces.
  • 37. The optical waveguide body of claim 33, wherein each of the plurality of optical features is an extraction feature.
  • 38. The optical waveguide body of claim 37, wherein each of the plurality of optical features is a curved protrusion.
  • 39. The optical waveguide body of claim 38, wherein the plurality of optical features is continuously formed.
CROSS REFERENCE TO RELATED APPLICATIONS

The present application claims the benefit of U.S. Provisional patent application Ser. No. 61/758,660, filed Jan. 30, 2013, entitled “Optical Waveguide” and owned by the assignee of the present application, and the disclosure of which is incorporated by reference herein.

US Referenced Citations (561)
Number Name Date Kind
3372740 Kastovich et al. Mar 1968 A
3532871 Shipman Oct 1970 A
4146297 Alferness et al. Mar 1979 A
4441787 Lichtenberger Apr 1984 A
4714983 Lang Dec 1987 A
4914553 Hamada et al. Apr 1990 A
4954930 Maegawa et al. Sep 1990 A
4977486 Gotoh Dec 1990 A
5005108 Pristash Apr 1991 A
5009483 Rockwell, III Apr 1991 A
5026161 Werner Jun 1991 A
5040098 Tanaka et al. Aug 1991 A
5047761 Sell Sep 1991 A
5061404 Wu et al. Oct 1991 A
5097258 Iwaki Mar 1992 A
5113177 Cohen May 1992 A
5113472 Gualtieri et al. May 1992 A
5165772 Wu Nov 1992 A
5171080 Bathurst Dec 1992 A
5175787 Gualtieri et al. Dec 1992 A
5186865 Wu et al. Feb 1993 A
5245689 Gualtieri Sep 1993 A
5253317 Allen et al. Oct 1993 A
5295019 Rapoport Mar 1994 A
5309544 Saxe May 1994 A
5359687 McFarland Oct 1994 A
5359691 Tai et al. Oct 1994 A
5396350 Beeson et al. Mar 1995 A
5398179 Pacheco Mar 1995 A
5400224 DuNah et al. Mar 1995 A
5428468 Zimmerman et al. Jun 1995 A
5461547 Ciupke et al. Oct 1995 A
5462700 Beeson et al. Oct 1995 A
5481385 Zimmerman et al. Jan 1996 A
5506924 Inoue Apr 1996 A
5521725 Beeson et al. May 1996 A
5521726 Zimmerman et al. May 1996 A
5528720 Winston et al. Jun 1996 A
5537304 Klaus Jul 1996 A
5541039 McFarland et al. Jul 1996 A
5548670 Koike Aug 1996 A
5553092 Bruce et al. Sep 1996 A
5555109 Zimmerman et al. Sep 1996 A
5555160 Tawara et al. Sep 1996 A
5555329 Kuper et al. Sep 1996 A
5572411 Watai et al. Nov 1996 A
5577492 Parkyn, Jr. et al. Nov 1996 A
5584556 Yokoyama et al. Dec 1996 A
5598280 Nishio et al. Jan 1997 A
5598281 Zimmerman et al. Jan 1997 A
5613751 Parker et al. Mar 1997 A
5613770 Chin, Jr. et al. Mar 1997 A
5657408 Ferm et al. Aug 1997 A
5658066 Hirsch Aug 1997 A
5659410 Koike et al. Aug 1997 A
5676453 Parkyn, Jr. et al. Oct 1997 A
5676457 Simon Oct 1997 A
5677702 Inoue et al. Oct 1997 A
5685634 Mulligan Nov 1997 A
5696865 Beeson et al. Dec 1997 A
5702176 Engle Dec 1997 A
5718497 Yokoyama et al. Feb 1998 A
5727107 Umemoto et al. Mar 1998 A
5735590 Kashima et al. Apr 1998 A
5739931 Zimmerman et al. Apr 1998 A
5748828 Steiner et al. May 1998 A
5761355 Kuper et al. Jun 1998 A
5769522 Kaneko et al. Jun 1998 A
5771039 Ditzik Jun 1998 A
5777857 Degelmann Jul 1998 A
5806955 Parkyn, Jr. et al. Sep 1998 A
5812714 Hulse Sep 1998 A
5818555 Yokoyama et al. Oct 1998 A
5839823 Hou et al. Nov 1998 A
5850498 Shacklette et al. Dec 1998 A
5854872 Tai Dec 1998 A
5863113 Oe et al. Jan 1999 A
5872883 Ohba et al. Feb 1999 A
5897201 Simon Apr 1999 A
5914759 Higuchi et al. Jun 1999 A
5914760 Daiku Jun 1999 A
5949933 Steiner et al. Sep 1999 A
5961198 Hira et al. Oct 1999 A
5967637 Ishikawa et al. Oct 1999 A
5974214 Shacklette et al. Oct 1999 A
5980054 Fukui Nov 1999 A
5997148 Ohkawa Dec 1999 A
5999281 Abbott et al. Dec 1999 A
5999685 Goto et al. Dec 1999 A
6007209 Pelka Dec 1999 A
6043951 Lee Mar 2000 A
6044196 Winston et al. Mar 2000 A
6079838 Parker et al. Jun 2000 A
6097549 Jenkins et al. Aug 2000 A
6134092 Pelka et al. Oct 2000 A
6139176 Hulse et al. Oct 2000 A
6151089 Yang et al. Nov 2000 A
6155692 Ohkawa Dec 2000 A
6155693 Spiegel et al. Dec 2000 A
6161939 Bansbach Dec 2000 A
6164790 Lee Dec 2000 A
6164791 Gwo-Juh et al. Dec 2000 A
6167182 Shinohara et al. Dec 2000 A
6206535 Hattori et al. Mar 2001 B1
6231200 Shinohara et al. May 2001 B1
6232592 Sugiyama May 2001 B1
6241363 Lee Jun 2001 B1
6257737 Marshall et al. Jul 2001 B1
6259854 Shinji et al. Jul 2001 B1
D446333 Fröis Aug 2001 S
6304693 Buelow, II et al. Oct 2001 B1
6310704 Dogan et al. Oct 2001 B1
6379016 Boyd et al. Apr 2002 B1
6379017 Nakabayashi Apr 2002 B2
6400086 Huter Jun 2002 B1
6421103 Yamaguchi Jul 2002 B2
6443594 Marshall et al. Sep 2002 B1
6461007 Akaoka Oct 2002 B1
6473554 Pelka et al. Oct 2002 B1
6480307 Yang Nov 2002 B1
6485157 Ohkawa Nov 2002 B2
6508563 Parker et al. Jan 2003 B2
6523986 Hoffmann Feb 2003 B1
6541720 Gerald et al. Apr 2003 B2
6554451 Keuper Apr 2003 B1
6568819 Yamazaki et al. May 2003 B1
6582103 Popovich et al. Jun 2003 B1
6585356 Ohkawa Jul 2003 B1
6598998 West et al. Jul 2003 B2
6612723 Futhey et al. Sep 2003 B2
6616290 Ohkawa Sep 2003 B2
6629764 Uehara Oct 2003 B1
6633722 Kohara et al. Oct 2003 B1
6634772 Yaphe et al. Oct 2003 B2
6647199 Pelka et al. Nov 2003 B1
6652109 Nakamura Nov 2003 B2
6659628 Gomez Del Campo Dec 2003 B2
6671452 Winston et al. Dec 2003 B2
6676284 Wynne Willson Jan 2004 B1
6678021 Ohkawa Jan 2004 B2
6679621 West et al. Jan 2004 B2
6712481 Parker et al. Mar 2004 B2
6724529 Sinkoff Apr 2004 B2
6724543 Chinniah et al. Apr 2004 B1
6727965 Kubota Apr 2004 B1
6752505 Parker et al. Jun 2004 B2
6755546 Ohkawa Jun 2004 B2
6758582 Hsiao et al. Jul 2004 B1
6775460 Steiner et al. Aug 2004 B2
6796676 Severtson et al. Sep 2004 B2
6802626 Belfer et al. Oct 2004 B2
6802628 Kuo Oct 2004 B2
6840656 Kuo Jan 2005 B2
6845212 Gardiner et al. Jan 2005 B2
6876408 Yamaguchi Apr 2005 B2
6894740 Ohkawa May 2005 B2
6896381 Benitez et al. May 2005 B2
6924943 Minano et al. Aug 2005 B2
D511221 Zucker Nov 2005 S
6974241 Hara et al. Dec 2005 B2
6992335 Ohkawa Jan 2006 B2
D518911 Lee Apr 2006 S
7025482 Yamashita et al. Apr 2006 B2
7046318 Yu et al. May 2006 B2
7046905 Gardiner et al. May 2006 B1
7063430 Greiner Jun 2006 B2
7072096 Holman et al. Jul 2006 B2
7083313 Smith Aug 2006 B2
7085460 Leu et al. Aug 2006 B2
7090370 Clark et al. Aug 2006 B2
7090389 Parker et al. Aug 2006 B2
7097341 Tsai Aug 2006 B2
7106528 Ohmori et al. Sep 2006 B2
7118253 Simon Oct 2006 B1
D532532 Maxik Nov 2006 S
7131764 Hsu et al. Nov 2006 B2
7152985 Benitez et al. Dec 2006 B2
7160010 Chinniah et al. Jan 2007 B1
7160015 Parker Jan 2007 B2
7168841 Hsieh et al. Jan 2007 B2
7175330 Chen Feb 2007 B1
7178941 Roberge et al. Feb 2007 B2
7182480 Kan Feb 2007 B2
7192174 Myoung Mar 2007 B2
7204634 Chen et al. Apr 2007 B2
7209628 Winston et al. Apr 2007 B2
7222995 Bayat et al. May 2007 B1
7223004 Chen et al. May 2007 B2
D544110 Hooker et al. Jun 2007 S
7246931 Hsieh et al. Jul 2007 B2
7265800 Jagt et al. Sep 2007 B2
7273299 Parkyn et al. Sep 2007 B2
7290906 Suzuki et al. Nov 2007 B2
7292767 Cheng Nov 2007 B2
D563036 Miyairi et al. Feb 2008 S
D565778 Pedersen Apr 2008 S
D566300 Lo Apr 2008 S
7364342 Parker et al. Apr 2008 B2
D568529 Colleran, Jr. et al. May 2008 S
D570025 Walker May 2008 S
D573292 Zheng et al. Jul 2008 S
7393124 Williams Jul 2008 B1
7399108 Ayabe et al. Jul 2008 B2
7400809 Erben et al. Jul 2008 B2
7404660 Parker Jul 2008 B2
D575898 Tran et al. Aug 2008 S
7407303 Wanninger et al. Aug 2008 B2
7422357 Chang Sep 2008 B1
D581555 To et al. Nov 2008 S
7458714 Chang Dec 2008 B2
7465074 Blumel Dec 2008 B2
D584838 To et al. Jan 2009 S
7486854 Van Ostrand et al. Feb 2009 B2
7488093 Huang et al. Feb 2009 B1
D587839 Guercio Mar 2009 S
D589195 Sabernig Mar 2009 S
7513672 Parker Apr 2009 B2
7520650 Smith Apr 2009 B2
7534013 Simon May 2009 B1
7559672 Parkyn et al. Jul 2009 B1
7566148 Noh et al. Jul 2009 B2
7566159 Oon et al. Jul 2009 B2
7581854 Ford Sep 2009 B2
D604002 Santoro Nov 2009 S
7614764 Williams et al. Nov 2009 B2
7626655 Yamazaki et al. Dec 2009 B2
7628508 Kita et al. Dec 2009 B2
7635205 Yu et al. Dec 2009 B2
7639918 Sayers et al. Dec 2009 B2
7641363 Chang et al. Jan 2010 B1
7648256 Shiratsuchi et al. Jan 2010 B2
D609384 Gray et al. Feb 2010 S
D610722 Bi Feb 2010 S
D612527 Espiau et al. Mar 2010 S
7674018 Holder et al. Mar 2010 B2
7703950 Ewert et al. Apr 2010 B2
7703967 Parker Apr 2010 B2
D615232 Xiao et al. May 2010 S
D616145 Boissevain May 2010 S
7710663 Barnes et al. May 2010 B2
7722224 Coleman et al. May 2010 B1
7722241 Chang May 2010 B2
7724321 Hsieh et al. May 2010 B2
D617489 Santoro Jun 2010 S
D618842 Ngai et al. Jun 2010 S
7736019 Shimada et al. Jun 2010 B2
7736045 Yamashita et al. Jun 2010 B2
7750982 Nelson et al. Jul 2010 B2
7753551 Yaphe et al. Jul 2010 B2
7758227 Coleman Jul 2010 B1
7760290 Kang et al. Jul 2010 B2
7762705 Sakai et al. Jul 2010 B2
D622894 Ngai et al. Aug 2010 S
7766515 Condon et al. Aug 2010 B2
7775697 Hirano Aug 2010 B2
7776236 Shih et al. Aug 2010 B2
7780306 Hoshi Aug 2010 B2
7784954 Coleman Aug 2010 B1
D623793 Ngai et al. Sep 2010 S
7798695 Parker Sep 2010 B2
D626260 Wei Oct 2010 S
7806581 Lee Oct 2010 B2
7810960 Soderman et al. Oct 2010 B1
7810968 Walker et al. Oct 2010 B1
7813131 Liang Oct 2010 B2
7821982 Chen et al. Oct 2010 B2
D627913 Gielen Nov 2010 S
D628319 Yoshinobu et al. Nov 2010 S
7826698 Meir et al. Nov 2010 B1
D629129 Lin et al. Dec 2010 S
7850357 Kim et al. Dec 2010 B2
7857619 Liu Dec 2010 B2
D630347 Pei et al. Jan 2011 S
D630775 Pan Jan 2011 S
D631577 Yoshinobu et al. Jan 2011 S
D631601 Lodhie Jan 2011 S
7866871 Couzin et al. Jan 2011 B2
D633636 Gielen Mar 2011 S
D634056 Hokzaono et al. Mar 2011 S
7905646 Adachi et al. Mar 2011 B2
7907804 Meir et al. Mar 2011 B2
7914192 Coleman Mar 2011 B2
7914193 Peifer et al. Mar 2011 B2
7914196 Parker et al. Mar 2011 B2
7929816 Meir et al. Apr 2011 B2
7934851 Boissevain et al. May 2011 B1
7967477 Bloemen et al. Jun 2011 B2
7969531 Li et al. Jun 2011 B1
D641923 Radchenko et al. Jul 2011 S
7976204 Li et al. Jul 2011 B2
D642725 Kong et al. Aug 2011 S
7991257 Coleman Aug 2011 B1
7997784 Tsai Aug 2011 B2
8002450 Van Ostrand et al. Aug 2011 B2
D645194 Budike, Jr. et al. Sep 2011 S
D646406 Tsai et al. Oct 2011 S
8033674 Coleman et al. Oct 2011 B1
8033706 Kelly et al. Oct 2011 B1
8038308 Greiner Oct 2011 B2
8047696 Ijzerman et al. Nov 2011 B2
8052316 Lee Nov 2011 B2
8054409 Hsieh et al. Nov 2011 B2
8061877 Chang Nov 2011 B2
8064743 Meir et al. Nov 2011 B2
8067884 Li Nov 2011 B2
8075157 Zhang et al. Dec 2011 B2
8087807 Liu et al. Jan 2012 B2
8092068 Parker et al. Jan 2012 B2
8096671 Cronk et al. Jan 2012 B1
8096681 Fang et al. Jan 2012 B2
D654618 Kong et al. Feb 2012 S
8113704 Bae et al. Feb 2012 B2
8128272 Fine et al. Mar 2012 B2
8129731 Vissenberg et al. Mar 2012 B2
8152339 Morgan Apr 2012 B2
8152352 Richardson Apr 2012 B2
8162524 Van Ostrand et al. Apr 2012 B2
D659880 Maxik et al. May 2012 S
8172447 Meir et al. May 2012 B2
8177408 Coleman May 2012 B1
8182128 Meir et al. May 2012 B2
8186847 Hu et al. May 2012 B2
D662255 Kluś Jun 2012 S
D662256 Kluś Jun 2012 S
D662643 Takahashi et al. Jun 2012 S
8192051 Dau et al. Jun 2012 B2
8198109 Lerman et al. Jun 2012 B2
8210716 Lerman et al. Jul 2012 B2
8218920 Van Ostrand et al. Jul 2012 B2
8220955 Kwak et al. Jul 2012 B2
8220980 Gingrich, III Jul 2012 B2
8226287 Teng et al. Jul 2012 B2
8231256 Coleman et al. Jul 2012 B1
8231258 Kim et al. Jul 2012 B2
8231259 Keller et al. Jul 2012 B2
8242518 Lerman et al. Aug 2012 B2
8246187 Cheong et al. Aug 2012 B2
8246197 Huang Aug 2012 B2
8249408 Coleman Aug 2012 B2
8258524 Tan et al. Sep 2012 B2
8272756 Patrick Sep 2012 B1
8272770 Richardson Sep 2012 B2
D668370 Guercio Oct 2012 S
8277106 Van Gorkom et al. Oct 2012 B2
8282261 Pance et al. Oct 2012 B2
8283853 Yan et al. Oct 2012 B2
8287152 Gill Oct 2012 B2
8297801 Coushaine et al. Oct 2012 B2
8297818 Richardson Oct 2012 B2
D670422 Siekmann Nov 2012 S
D670856 Butler et al. Nov 2012 S
8314566 Steele et al. Nov 2012 B2
8317363 Zheng Nov 2012 B2
8317366 Dalton et al. Nov 2012 B2
8319130 Lee et al. Nov 2012 B2
8325292 Ouchi Dec 2012 B2
8328403 Morgan et al. Dec 2012 B1
8328406 Zimmermann Dec 2012 B2
8331746 Bogner et al. Dec 2012 B2
8338199 Lerman et al. Dec 2012 B2
8338839 Lerman et al. Dec 2012 B2
8338840 Lerman et al. Dec 2012 B2
8338841 Lerman et al. Dec 2012 B2
8338842 Lerman et al. Dec 2012 B2
8344397 Lerman et al. Jan 2013 B2
8348446 Nakamura Jan 2013 B2
8353606 Jeong Jan 2013 B2
8369678 Chakmakjian et al. Feb 2013 B2
8382354 Kim et al. Feb 2013 B2
8382387 Sandoval Feb 2013 B1
D677806 Jiang et al. Mar 2013 S
8388173 Sloan et al. Mar 2013 B2
8388190 Li et al. Mar 2013 B2
8398259 Kwak et al. Mar 2013 B2
8398262 Sloan et al. Mar 2013 B2
D679437 Watt Apr 2013 S
D679444 Vasylyev Apr 2013 S
D679843 Hsu et al. Apr 2013 S
D681262 Lee Apr 2013 S
8408737 Wright et al. Apr 2013 B2
8410726 Dau et al. Apr 2013 B2
8412010 Ghosh et al. Apr 2013 B2
8414154 Dau et al. Apr 2013 B2
8419224 Wan-Chih et al. Apr 2013 B2
8430536 Zhao Apr 2013 B1
8430548 Kelly et al. Apr 2013 B1
8432628 Shiau et al. Apr 2013 B2
8434892 Zwak et al. May 2013 B2
8434893 Boyer et al. May 2013 B2
8434913 Vissenberg et al. May 2013 B2
8434914 Li et al. May 2013 B2
8449128 Ko et al. May 2013 B2
8449142 Martin et al. May 2013 B1
D684296 Henderson et al. Jun 2013 S
8454218 Wang et al. Jun 2013 B2
8461602 Lerman et al. Jun 2013 B2
8469559 Williams Jun 2013 B2
8475010 Vissenberg et al. Jul 2013 B2
8485684 Lou et al. Jul 2013 B2
8506112 Dau et al. Aug 2013 B1
8534896 Boonekamp Sep 2013 B2
8534901 Panagotacos et al. Sep 2013 B2
8547022 Summerford et al. Oct 2013 B2
8567983 Boyer et al. Oct 2013 B2
8567986 Szprengiel et al. Oct 2013 B2
D694449 Walker Nov 2013 S
8573823 Dau et al. Nov 2013 B2
8585253 Duong et al. Nov 2013 B2
8593070 Wang et al. Nov 2013 B2
D695442 Speier et al. Dec 2013 S
D695447 Speier et al. Dec 2013 S
8598778 Allen et al. Dec 2013 B2
8602586 Dau et al. Dec 2013 B1
8608351 Peifer Dec 2013 B2
8632214 Tickner et al. Jan 2014 B1
8641219 Johnson et al. Feb 2014 B1
8657479 Morgan et al. Feb 2014 B2
8724052 Hsieh et al. May 2014 B2
8740440 Mizuno et al. Jun 2014 B2
8755005 Bierhuizen et al. Jun 2014 B2
8833999 Wang et al. Sep 2014 B2
8864360 Parker et al. Oct 2014 B2
8870431 Lin et al. Oct 2014 B2
8882323 Solomon et al. Nov 2014 B2
8905569 Thomas et al. Dec 2014 B2
8915611 Zhang Dec 2014 B2
8917962 Nichol et al. Dec 2014 B1
20010019479 Nakabayashi et al. Sep 2001 A1
20020061178 Winston et al. May 2002 A1
20020172039 Inditsky Nov 2002 A1
20030034985 Needham Riddle et al. Feb 2003 A1
20040008952 Kragl Jan 2004 A1
20040080938 Holman et al. Apr 2004 A1
20040135933 Leu et al. Jul 2004 A1
20040213003 Lauderdale et al. Oct 2004 A1
20040240217 Rice Dec 2004 A1
20050111235 Suzuki et al. May 2005 A1
20050210643 Mezei et al. Sep 2005 A1
20060002146 Baba Jan 2006 A1
20060262521 Piepgras et al. Nov 2006 A1
20070081780 Scholl Apr 2007 A1
20070086179 Chen et al. Apr 2007 A1
20070121340 Hoshi May 2007 A1
20070139905 Birman et al. Jun 2007 A1
20070189033 Watanabe et al. Aug 2007 A1
20070245607 Awai et al. Oct 2007 A1
20070253058 Wood Nov 2007 A1
20070274654 Choudhury et al. Nov 2007 A1
20080037284 Rudisill Feb 2008 A1
20080137695 Takahashi et al. Jun 2008 A1
20080186273 Krijn et al. Aug 2008 A1
20080192458 Li Aug 2008 A1
20080199143 Turner Aug 2008 A1
20090103293 Harbers et al. Apr 2009 A1
20090257242 Wendman Oct 2009 A1
20090297090 Bogner et al. Dec 2009 A1
20090309494 Patterson et al. Dec 2009 A1
20100008088 Koizumi et al. Jan 2010 A1
20100027257 Boonekamp et al. Feb 2010 A1
20100046219 Pijlman et al. Feb 2010 A1
20100073597 Bierhuizen et al. Mar 2010 A1
20100079843 Derichs et al. Apr 2010 A1
20100079980 Sakai Apr 2010 A1
20100128483 Reo et al. May 2010 A1
20100133422 Lin et al. Jun 2010 A1
20100157577 Montgomery et al. Jun 2010 A1
20100208460 Ladewig et al. Aug 2010 A1
20100220484 Shani et al. Sep 2010 A1
20100220497 Ngai Sep 2010 A1
20100231143 May et al. Sep 2010 A1
20100238645 Bailey Sep 2010 A1
20100238671 Catone et al. Sep 2010 A1
20100302218 Bita et al. Dec 2010 A1
20100302616 Bita et al. Dec 2010 A1
20100302783 Shastry et al. Dec 2010 A1
20100302803 Bita et al. Dec 2010 A1
20100328936 Pance et al. Dec 2010 A1
20110007505 Wang Jan 2011 A1
20110037388 Lou et al. Feb 2011 A1
20110058372 Lerman et al. Mar 2011 A1
20110063830 Narendran et al. Mar 2011 A1
20110063838 Dau et al. Mar 2011 A1
20110163681 Dau et al. Jul 2011 A1
20110163683 Steele et al. Jul 2011 A1
20110170289 Allen et al. Jul 2011 A1
20110180818 Lerman et al. Jul 2011 A1
20110193105 Lerman et al. Aug 2011 A1
20110193106 Lerman et al. Aug 2011 A1
20110193114 Lerman et al. Aug 2011 A1
20110195532 Lerman et al. Aug 2011 A1
20110198631 Lerman et al. Aug 2011 A1
20110198632 Lerman et al. Aug 2011 A1
20110199769 Bretschneider et al. Aug 2011 A1
20110204390 Lerman et al. Aug 2011 A1
20110204391 Lerman et al. Aug 2011 A1
20110210861 Winton et al. Sep 2011 A1
20110228527 Van Gorkom et al. Sep 2011 A1
20110233568 An et al. Sep 2011 A1
20110249467 Boonekamp Oct 2011 A1
20110273882 Pickard Nov 2011 A1
20110280043 Van Ostrand et al. Nov 2011 A1
20110299807 Kim et al. Dec 2011 A1
20110305018 Angelini et al. Dec 2011 A1
20110305027 Ham Dec 2011 A1
20110317436 Kuan Dec 2011 A1
20120008338 Ono et al. Jan 2012 A1
20120026728 Lou et al. Feb 2012 A1
20120033445 Desmet et al. Feb 2012 A1
20120039073 Tong Feb 2012 A1
20120051041 Edmond et al. Mar 2012 A1
20120068615 Duong Mar 2012 A1
20120069579 Koh Mar 2012 A1
20120069595 Catalano Mar 2012 A1
20120113676 Van Dijk et al. May 2012 A1
20120114284 Ender May 2012 A1
20120120651 Peck May 2012 A1
20120152490 Wen et al. Jun 2012 A1
20120170266 Germain et al. Jul 2012 A1
20120170316 Lee et al. Jul 2012 A1
20120170318 Tsai et al. Jul 2012 A1
20120182767 Petcavich et al. Jul 2012 A1
20120250296 Lu et al. Oct 2012 A1
20120250319 Dau et al. Oct 2012 A1
20120257383 Zhang Oct 2012 A1
20120268931 Lerman et al. Oct 2012 A1
20120268932 Lerman et al. Oct 2012 A1
20120287619 Pickard et al. Nov 2012 A1
20120287654 He et al. Nov 2012 A1
20120298181 Cashion et al. Nov 2012 A1
20120320626 Quilici et al. Dec 2012 A1
20130010464 Shuja et al. Jan 2013 A1
20130028557 Lee et al. Jan 2013 A1
20130037838 Speier et al. Feb 2013 A1
20130038219 Dau et al. Feb 2013 A1
20130039050 Dau et al. Feb 2013 A1
20130044480 Sato et al. Feb 2013 A1
20130077298 Steele et al. Mar 2013 A1
20130128593 Luo May 2013 A1
20130170210 Athalye Jul 2013 A1
20130201715 Dau et al. Aug 2013 A1
20130208461 Warton et al. Aug 2013 A1
20130208495 Dau et al. Aug 2013 A1
20130214300 Lerman et al. Aug 2013 A1
20130215612 Garcia Aug 2013 A1
20130223057 Gassner et al. Aug 2013 A1
20130229804 Holder et al. Sep 2013 A1
20130229810 Pelka et al. Sep 2013 A1
20130250584 Wang et al. Sep 2013 A1
20130279198 Lin et al. Oct 2013 A1
20130294059 Galluccio et al. Nov 2013 A1
20130294063 Lou et al. Nov 2013 A1
20130343045 Lodhie et al. Dec 2013 A1
20130343055 Eckert et al. Dec 2013 A1
20130343079 Unger et al. Dec 2013 A1
20140003041 Dau et al. Jan 2014 A1
20140029257 Boyer et al. Jan 2014 A1
20140071687 Tickner et al. Mar 2014 A1
20140168955 Gershaw Jun 2014 A1
20140268879 Mizuyama et al. Sep 2014 A1
20140334126 Speier et al. Nov 2014 A1
20150003059 Haitz et al. Jan 2015 A1
Foreign Referenced Citations (22)
Number Date Country
20014114 Dec 2000 DE
20107425 Jul 2001 DE
10047101 May 2002 DE
10203106 Jul 2003 DE
10302563 Jul 2004 DE
10302564 Jul 2004 DE
102006009325 Sep 2007 DE
102006011296 Sep 2007 DE
102006013343 Sep 2007 DE
1167870 Jan 2002 EP
H 10173870 Jun 1998 JP
2000147264 May 2000 JP
3093080 Dec 2005 JP
WO 9621122 Jul 1996 WO
WO 9621884 Jul 1996 WO
WO 9904531 Jan 1999 WO
WO 03031869 Apr 2003 WO
WO 2008102655 Aug 2008 WO
WO 2009012484 Jan 2009 WO
WO 2011130648 Oct 2011 WO
WO 2013078463 May 2013 WO
WO 2013082537 Jun 2013 WO
Non-Patent Literature Citations (17)
Entry
Web page at http://www.fusionoptix.com/lighting/components/array-optics.htm, printed May 9, 2013 (2 pages).
U.S. Appl. No. 13/657,421, filed Oct. 22, 2012 (38 pages).
Web page at http://www.oluce.com/en/lamps/table/colombo-281-detail, printed Nov. 19, 2013 (2 pages).
International Search Report and Written Opinion dated Jul. 10, 2014, for International Application No. PCT/US2014/013400, Applicant, Cree, Inc. (21 pages).
Invitation to Pay Additional Fees dated Apr. 30, 2014, for International Application No. PCT/US2014/013400, Applicant, Cree, Inc. (2 pages).
International Search Report and Written Opinion dated Jul. 10, 2014, for International Application No. PCT/US2014/013934, Applicant, Cree, Inc. (19 pages).
Invitation to Pay Additional Fees dated May 1, 2014, for International Application No. PCT/US2014/013934, Applicant, Cree, Inc. (2 pages).
International Search Report and Written Opinion dated Jul. 24, 2014, for International Application No. PCT/US2014/28887, Applicant, Cree, Inc. (15 pages).
International Search Report and Written Opinion dated Jul. 28, 2014, for International Application No. PCT/US2014/28938, Applicant, Cree, Inc. (19 pages).
International Search Report and Written Opinion dated Jul. 14, 2014, for International Application No. PCT/US2014/013931 Applicant, Cree, Inc. (21 pages).
International Search Report and Written Opinion for International Application No. PCT/US2014/013854, issued Jun. 5, 2014, Applicant, Cree, Inc. (15 pages).
Drain, Kieran, “Transformations in Lighting: 2011 DOE Solid-State Lighting R&D Workshop, Panel 3: Novel Lighting Concepts for Large Interior Spaces,” PowerPoint presentation, Nov. 2013 (23 pages).
Ji et al., “Electrically Controllable Microlens Array Fabricated by Anisotropic Phase Separation From Liquid-Crystal and Polymer Composite Materials,” vol. 28, No. 13, Optics Letters, pp. 1147-1149, Jul. 1, 2003 (4 pages).
Iijima., et al., “Document Scanner Using Polymer Waveguides With a Microlens Array,” Optical Engineering, vol. 41, Issue 11, pp. 2743-2748, Oct. 28, 2002 (4 pages).
Invitation to Pay Additional Fees dated May 1, 2014, for International Application No. PCT/US2014/013931, Applicant: Cree, Inc. (2 pages).
International Search Report and Written Opinion for International Application No. PCT/US2014/013408, issued Jul. 17, 2014, Applicant, Cree, Inc. (21 pages).
Invitation to Pay Additional Fees for International Application No. PCT/US2014/013408, issued May 8, 2014, Applicant, Cree, Inc. (2 pages).
Related Publications (1)
Number Date Country
20140212090 A1 Jul 2014 US
Provisional Applications (1)
Number Date Country
61758660 Jan 2013 US