Abstract:
A light emitting device includes a base; a light emitting diode (LED) supported by the base; a layer spaced apart from the LED and including a light emitting material of refraction index n 1 . An enclosure formed by the layer and the base encloses the LED. A medium inside the enclosure between the LED and the layer has a refraction index n 0 &lt;n 1 ; and an optic in contact with the layer and having a refraction index n 2 ≧n 1 . The layer is positioned between the optic and the LED. The optic has, at a surface of contact with the layer, a radius r measured along a ray originating from the LED, and, at an output surface of the optic, another radius R measured along the same ray, such that R≧r·(n 1 /n m ), where n m  is a refraction index of a medium adjacent the output surface of the optic.

Description:
CROSS-REFERENCE TO RELATED APPLICATIONS 
       [0001]    This application claims the benefit of U.S. Provisional Application No. 60/961,185, filed Jul. 19, 2007, which is hereby incorporated by reference herein in its entirety. 
     
    
     TECHNICAL FIELD 
       [0002]    The present invention relates generally to the field of solid-state lighting and more specifically to high efficiency phosphor-converted LEDs. 
       BACKGROUND 
       [0003]    Solid-state lighting (SSL) is a type of lighting that does not use an electrical filament or a gas in the production of light. A primary advantage of SSL over conventional lighting technologies is the potential energy savings as a result of its higher luminous efficiencies over conventional lighting devices. For example, SSL is capable of 50% efficiency with 200 lumen per watt (lm/W) efficacy (compared to 15 lm/W for incandescents and 60-90 lm/W for fluorescents) and up to 100 khr lifetimes. This is approximately 100 times the lifetime of conventional incandescent bulbs and 10 times the lifetime of fluorescents. The Department of Energy (DOE) has set a goal of 50% electrical-to-optical system efficiency with a spectrum accurately reproducing the solar spectrum by 2020. The Optoelectronic Industry Development Association (OIDA) aims for 200-lm/W luminous efficiency with a color rendering index greater than 80. 
         [0004]    Each of these conventional methods and devices has deficiencies. Color mixing is hindered by the absence of an efficient LED material in the 500 nm to 580 nm (green-to-yellow) range. Wavelength conversion suffers from phosphor conversion loss and package designs that do not extract phosphor-converted light efficiently. 
         [0005]    SSL devices primarily include light emitting diodes (LEDs), which include a small chip semiconductor, i.e. the LED source, mounted in a reflector cup on a lead frame. The LED source generates photons of light at a first wavelength when energized. The reflector cup reflects photons out of the LED. An optic, generally a silicone or epoxy encapsulation, aids in light extraction from the LED source and protects the LED components. 
         [0006]    High efficiency generation of white light with LEDs has conventionally been according to one of three methods: 1) color mixing; 2) wavelength conversion; or 3) a combination of methods 1 and 2. Color mixing is the use of multiple LEDs across the visible spectrum (e.g. blue+green+red LEDs), which combine to produce a white light. Wavelength conversion is the use of a single, efficient, short wavelength LED emitting light at the first wavelength, which is then at least partially absorbed by a phosphor within the LED and re-emitted at a second wavelength, LEDs under method  2  are generally referred to as phosphor-converted LEDs (pcLEDs). 
         [0007]    Conventional pcLEDs have generally two structural arrangements. First, the phosphor can encompass the LED source of the LED. The phosphor is typically a YAG:Ce crystalline powder in direct contact with the blue wavelength emitting LED source. Both are positioned upon a heat sink base and surrounded by an optic. The other arrangement is a scattered photon extraction (SPE) pcLED, which positions a planar phosphor-layer at a distance away from the LED source. Herein, the YAG:Ce phosphor, in powder form, creates a diffuse, semitransparent layer upon an acrylic optic with a planar surface. 
         [0008]    When the phosphor is in direct contact with the LED source, the phosphor suffers from optical losses by reflection of phosphor-emission back into the LED source rather than through the optic and out of the LED. This can account for up to 60% of the total phosphor emission. The SPE pcLED suffers from scattering of the phosphor emissions. Scattering is the result of substantial differences in the indices of refraction of the phosphor powder and the material that encapsulates the phosphor (air, silicon, PMMA, or glass). The index of refraction, n, is a measure, of the relative speed of light in a medium as compared to in a vacuum (where n vac =1). When light passes from one medium to another medium with a substantially different index of refraction, the speed and direction of the light changes and is known as refraction. Refraction can lead to a randomization, or scattering, of the directionality of the light. Scattering then reduces efficiency by increasing the path length (a) inside the phosphor layer by trapping of the emissions by total internal reflection and (b) inside the device package because of random directionality of the phosphor emission, both of which can lead to reabsorption and optical loss. 
         [0009]    These phosphor-related deficiencies are then compounded by secondary losses encountered by other package design deficiencies, such as imperfections of the reflector cup within the LED. While the reflector cup is intended to direct the phosphor-emission out of the LED, internal reflections and path randomization can trap a portion of the phosphor-emission, such as between the reflector cop and the phosphor, and decrease LED efficiency by approximately 30%. 
         [0010]    Thus, to reach the efficiency goals set forth by the DOE, the problems associated with package design must be eliminated by designing a high efficiency LED that resolves the issues identified above. 
       SUMMARY OF THE INVENTION 
       [0011]    According to the embodiments of the present invention, a light emitting composite material is described. The light emitting composite material includes a glassy material and a plurality of phosphor particles suspended within the glassy material, wherein the refractive index of the plurality of phosphor particles is approximately equal to the refractive index of the glassy material. 
         [0012]    The plurality of phosphor particles can be composed of an inorganic crystalline material selected from the group consisting of Y x Gd y Al v Ga w O 12 :M 3+ , wherein x+y=3 and v+w=5; SrGa 2 S 4 :M 2+ ; SrS:M 2+ ; X 2 Si 5 Ng:M 2+ ; and XSi 2 O 2 N 2 :M 2+ , wherein X is selected from a group consisting of Be, Mg, Ca, Sr, and Ba and wherein M is selected from a group consisting of Ce, Eu, Mn, Nd Pr, Sm, Gd, Tb, Dy, Ho, Er, Tm, Yb, Lu, Sc, Ti, V, Cr, Fe, Co, Ni, Cu, Zn, Ir, and PL. 
         [0013]    The glassy material can be an optical glass comprising an amount from 5% to about 35% of SiO 2 ; an amount from about 55% to about 88% of PbO; optionally an amount less than 10% B 2 O 3 ; optionally a combined amount less than 8% of Na 2 O and K 2 O; and optionally a combined amount less than about 15% total of TiO 2 , ZrO 2 , La 2 O 3 , and ZnO, and BaO. 
         [0014]    In other light emitting composites, the glassy material can be an optical glass comprising an amount from about 21% to about 30% of TiO 2 ; an amount from about 30% to about 50% of BaO, NaO, BeO, CaO, SrO, CdO, Ga 2 O 3 , In 2 O 3 , or Y 2 O 3 ; an amount from about 18% to about 24% of Al 2 O 3 ; and an amount from about 1% to about 10% of SiO 2 , B 2 O 3 , PbO, GeO 2 , SnO 2 , ZrO 2 , HfO 2 , ThO 2 . 
         [0015]    In another aspect of the present invention, the light emitting composites of the present invention can be used within a phosphor-containing light emitting device (pcLED). The pcLED can be constructed as an Enhanced Light Extraction by Internal Reflection (ELIXIR) LED device. 
         [0016]    In yet another aspect of the present invention, the light emitting composite can be used with a solid-state laser. 
         [0017]    In yet another aspect of the present invention, the light emitting composite can be used as a luminescence collector. 
     
    
     
       BRIEF DESCRIPTION OF THE FIGURES 
         [0018]      FIG. 1  is a diagrammatic cross-sectional view of the ELIXIR LED device according an embodiment of the present invention. 
           [0019]      FIG. 2  is a sample spectrum demonstrating the LED source emission band, the phosphor absorption band, and the phosphor emission band. 
           [0020]      FIG. 3  is a diagrammatic cross-sectional view of the ELIXIR LED device according to another embodiment of the present invention. 
           [0021]      FIG. 4  is an enlarged diagrammatic cross-sectional view of a nearly-indexed matched luminescent glass crystal composite. 
           [0022]      FIG. 5A  is a diagrammatic cross-sectional view of the total internal reflections within a conventional pcLED device. 
           [0023]      FIG. 5B  is a diagrammatic cross-sectional view that illustrates the relation between the relative radii of first and second materials, which leads to total internal reflection. 
           [0024]      FIG. 6  is a diagrammatic view of a conventional pumped solid-state laser device. 
           [0025]      FIG. 7  is a diagrammatic view of a pumped solid-state laser device according to an embodiment of the present invention. 
           [0026]      FIG. 8  is a diagrammatic view of a luminescence collector according to an embodiment of the present invention. 
           [0027]      FIG. 9  is a diagrammatic cross-sectional view of the result of a ray trace diagram for the ELIXIR LED device according to one embodiment of the present invention. 
       
    
    
     DETAILED DESCRIPTION 
       [0028]    Efficiency of a fully wavelength converted pcLED can he expressed as 
         [0000]      η poL =η LED ·η s ·η q ·η p   Equation 1
 
         [0000]    where η poL  is the total pcLED efficiency and is dependent upon the efficiency of the particular LED source, η LED ; the Stokes conversion efficiency, η s , which is the quantum ratio of the average emission wavelengths of the LED and the phosphor; the phosphor quantum efficiency, η q , which indicates the efficiency of the quantum conversion of light from a first wavelength to a second wavelength inside the phosphor; and the package efficiency, η p , which is the efficiency of light extraction of LED- and phosphor-emitted photons from the LED device package. The product of η q ·η p  is the conversion efficiency (CE) for an LED device. The embodiments of the present invention optimize CE. 
         [0029]    Package efficiency, η p , of the present invention is improved over conventional LED devices by first separating an LED source  12  from first and second non-planar layers, wherein the second layer is composed of a phosphor  14 , which will nearly eliminate the reflection of phosphor- and LED-emissions back into the LED source  12 . Secondly, a planar reflector  16  is used to reduce the number of mirror reflections over the conventional LED. The result is an Enhanced Light eXtraction by Internal Reflection (ELIXIR) LED device  10 , shown in  FIG. 1 . 
         [0030]    The ELIXIR LED  10  more specifically includes the first non-planar layer, i.e. a glass cover  18 , surrounding and making immediate contact with the second non-planar layer, i.e. a phosphor  14 , and a LED source  12  upon a heat sink base  20 . The phosphor  14  and the LED source  12  are separated by a radius sufficient to substantially reduce the likelihood of phosphor-emissions reentering the LED source  12 . This distance, r, is dependent upon a specified fraction of reentry, P, and is given by: 
         [0000]        r≧✓[A/ (4·π· P )]  Equation 2
 
         [0000]    Herein, A is the size of the LED source  12 , i.e. the surface area of the LED chip. 
         [0031]    The LED source  12  can include any conventional resonance cavity LED or laser diode source generally emitting a light having a first wavelength ranging between about 350 nm to about 500 nm. This can include, but should not be limited to, a blue power LED with a peak wavelength of 455 nm with a 1000 mA DC drive capability. 
         [0032]    The glass cover  18  can be any material suitable for the lens construction and for protection of the phosphor  14  and LED source  12 , such as polymethyl methacrylate (PMMA), silicones, and glasses. In an alternative embodiment described herein, the glass cover  18  and the phosphor  14  may be made integral. 
         [0033]    The phosphor  14  is applied to the glass cover  18  as a layer of inorganic phosphor crystalline powder. The phosphor  14  can be applied as a layer, for example, of about 100 μm in thickness, to an inner surface of the glass cover  18  from a solution of acetone or other solvent. The phosphor  14  should be selected such that the phosphor absorption band substantially overlaps with the LED-emission band, as shown in  FIG. 2 . This ensures efficient transfer front the first wavelength, the LED-emission, to the second wavelength, the phosphor-emission. Thus, a suitable phosphor for use with the blue power LED source can be Johnson Polymer Joncryl 587 modified styrene acrylic with 0.2% BASF Lumogen. F Yellow 083 fluorescent dye. 
         [0034]    Though not specifically shown, the glass cover  18  can be eliminated and the phosphor  14  is applied as a layer upon the inside radius of a hemispherical optic  22 . 
         [0035]    While the phosphor  14 , glass cover  18 , and optic  22  are generally illustrated and explained with a hemispherical shape, the shape should not be considered so limited. That is, the shape can include hemispheres (see  FIG. 1 ), ellipsoids, spheres  24  (see  FIG. 3 ), or other similar shapes as is desired or necessary. In this way, the phosphor  26 , glass cover  28 , and optic  30  will include an opening  34  for electrical connections  36  and support  38  to the LED source  32 . While not necessary, the opening  34  should he small in construction to further minimize emission losses. 
         [0036]    In optimizing η 4  of Equation 1 and the ELIXIR LED  10  of  FIG. 1 , the phosphor  14  and glass cover  18  are replaced with a light emitting composite material  40  of  FIG. 4 . The light emitting composite material  40  integrates the first and second non-planar layers as an inorganic crystalline  42  suspended in a glassy material  44  matrix as illustrated in  FIG. 4 . The inorganic crystalline  42  and glassy material  44  are selected such that, n c , the index of refraction of the inorganic crystalline  42  is approximately equal, n g , to the index of refraction of the glassy material  44 . The result is a nearly index-matched luminescent glass-crystal composite (NIMLGCC)  40  that maximizes the quantum efficiency of the phosphor by reducing, or eliminating, optical scattering. 
         [0037]    Because of their large surface-to-volume ratio, nanoparticles have low quantum efficiencies. Thus, the inorganic crystalline  42  should be a particle  46  that is larger than about 10 nm, i.e. not a nanoparticle. However, because the light-emitting composite material  40  has a finite thickness, the inorganic crystalline  42  should be smaller than the thickness of the light-emitting composite material  40 . Suitable inorganic crystalline  42  can include Y x Gd y Al v Ga w O 12 :M 3+ , wherein x+y=3 and v+w=5; SrGa 2 S 4 :M 3+ ; SrS:M 3+ ; X 2 Si 5 N 8 :M 2+ ; and XSi 2 O 2 N 2 :M 2+ , wherein X is selected from a group consisting of Be, Mg, Ca, Sr, and Ba and wherein M is selected from a group consisting of Ce, Eu, Mn, Nd, Pr, Sm, Gb, Tb, Dy, Hu, Er, Tm, Yb, Lu, Sc, Ti, V, Cr, Fe, Co, Ni, Cu, Zn, Ir, and Pt. 
         [0038]    It would be permissible for the light-emitting composite material  40  to comprise a combination of different inorganic crystallines  42  to Obtain a color mixing result of broadband white light emission. For example, two or more UV- or violet-short wavelength inorganic crystalline materials  42  in the 350 nm to 430 nm range will absorb the first wavelength from the LED source  12  and reemit a combination of red, green, and blue light to achieve a broadband white. The broadband white resulting from a color-mixing light-emitting composite  40  is more highly uniform as compared to conventional phosphor color mixing because the emissions of red, green, and blue originate from the same location. In another example, where blue or blue-green short wavelength LED sources  12  are used (430 nm to 500 nm), these inorganic crystalline materials  42  will reemit the first wavelength in combination with red and green light to achieve a broadband white. 
         [0039]    The glassy material  44  in which the inorganic crystalline material is suspended can include an optical glass or other glass material, such as those manufactured by Schott North America (Elmsford, N.Y.) including SF-57, SF-67, LASF-9, LASF047, SK-57, PK-51, PK-53, FK-51A, and PK-5. Other optical glasses can include those according to the teachings of U.S. Appl. No. 2005/0075234 or U.S. Pat. No. 3,960,509, which are hereby incorporated by reference, in their entirety. 
         [0040]    The glassy material  44  can comprise about 10% to about 99.9% of the light-emitting composite material  40  by weight. 
         [0041]    As indicated above, the selection of an inorganic crystalline  42  and glassy material  44  should be according to index-matching. That is, the index of refraction, n o  of the inorganic crystalline  42  should be approximately equal to the index of refraction, n g , of the glassy material to provide an index of refraction, n 2 , for the light-emitting composite materiel  40 . 
         [0042]    By nearly index-matching the inorganic crystalline  42  to the glassy material  44 , scattering induced loss is nearly eliminated. That is, by establishing an n g  that is approximately equal to n c  , the phosphor-emission will travel at a speed within the inorganic crystalline  42  that is approximately equal to the travel speed within the glassy material  44  and thus reduce refraction, or a change in the direction of the emission. As a result, scattering is reduced and η p  increased. 
         [0043]    Total internal reflections  48  occur when the interface between first and second material  52 ,  54  cannot be traversed by light, as illustrated with a conventional LED device  50  in  FIG. 5 . This condition at the interface occurs when the refractive index of the first material  52  (here the phosphor) is greater than the refractive index of the second material  54 . According to Snell&#39;s Law, the light cannot traverse the interface, but will either refract along the interface or undergo total internal reflection. Total internal reflection  48  of the emission  58  continues until all of the energy in the emission is reabsorbed  60  by the phosphor. 
         [0044]    Thus, Snell&#39;s Law can be used to calculate a radius at which total internal reflections  48  are eliminated. This radius is determinable by establishing a ratio of a radius to the light-emitting composite material  40 , r, to a radius to the outer diameter of the light-emitting composite material, R. This ratio of radii must be less than or equal to the ratio of the index of refraction for material external to the ELIXIR LED device  10 , n 1 , and n 2 : 
         [0000]        r/R≦n   1   /n   2   Equation 3
 
         [0000]    Often, this material external to the ELIXIR LED  10  will be air, or vacuum, having n 1 =1. Thus, total internal reflections  48  will be avoided when r/R is less than the inverse of n 2 . 
         [0045]    The ELIXIR LED  10  of  FIG. 9  includes the light-emitting composite material  40  positioned upon the planar reflector  16  as provided by Equation 3. Materials for the planar reflector  16  can include aluminized Mylar attached to an acrylic sheet or a 3M Vikuiti enhanced specular reflector film. By eliminating the reflector cup of conventional LED package design, phosphor-emission can leave the ELIXIR LED  10  without being trapped between the reflector cup and the phosphor. 
         [0046]    Finally, the optic  22  positioned externally to the light-emitting composite material  40  can be constructed of a glass material similar to the glassy material  44  of the light-emitting composite material  40 . Other materials can also be used so long as refractive index of the optic  22  is greater than or equal to n 2 . Suitable materials for the optic  22  construction can be polymethyl methacrylate (PMMA), silicones, and glasses having refractive indices of about 1.3 to about 2.2. 
         [0047]    When PMMA is used in constructing the optic  22 , the method can include polymerization of a methyl methacrylate monomer around a 25 mL round bottom flask to form an inner radius of the optic  22  with an inner diameter of approximately 3.8 cm. The outer diameter of the optic  22  can be shaped, for example, by an aluminum mold. However, other fabrication methods would be known and the size could be varied according to a particular need. 
         [0048]    The monomer for constructing the optic  22  can be purified to eliminate Contaminants. For PMMA, the methyl methacrylate monomer can be washed with a solution of sodium hydroxide, rinsed with deionized water, and dried with anhydrous magnesium sulfate. Polymerization can be initiated by benzoyl peroxide and heating the solution to 90° C. The resultant viscous solution is then poured into a mold, such as the one described previously, and then cured in an oven at 35° C. for one week. 
         [0049]    The optic  22  could also be produced with a high quality injection molding of PMMA rather than polymerization. 
         [0050]    While the ELIXIR LED  10  of  FIG. 9  is generally shown to include an air gap  62 , it would be understood that the air gap  62  can be partially, or completely, replaced with a glass or polymer having an refractive index less than or equal to n 2 . 
         [0051]    In other embodiments, the NIMLGCC can be used with visible diode-pumped solid-state lasers  84  as illustrated in  FIG. 7 . Conventional diode-pumped solid-state lasers  64  (see  FIG. 6 ) include a light source  66  comprising a power source  68  providing energy to a diode pump  70 , such as AlGaAs laser diode. Photons emitted from the diode pump  70  are directed into a laser cavity  74  by a fiber  72 . The photons entering the laser cavity  74  are directed to a population inversion crystal  76 , such as a YAG:Nd, which when excited by the photons will emit a light at a first wavelength (at 1064 nm). Light of this first wavelength can then reflect between input and output mirrors  78 ,  80  and yield a coherent emission, characteristic of the solid-state laser  64 . A portion of the first wavelength will impact a doubling crystal  82 , such as a potassium titanium oxide phosphate (KTP) crystal, which doubles the frequency of the light (conversion of the first wavelength to a second wavelength equal to 532 nm). Light of the second wavelength is not reflected by the output mirror  80 , but rather passes through the output mirror  80  at the laser output. 
         [0052]    However, the YAG:Nd population inversion crystal  76  said KTP doubling crystal  82  are a highly expensive component of the conventional pumped solid-state laser  64 . The NIMLGCC, as explained above, can provide an economical and energetically efficient alternative to the conventional pumped solid-state laser  64 . 
         [0053]    For example, as in  FIG. 7 , the YAG:Nd population inversion crystal  76  and NTP doubling crystal  82  are replaced by an NIMLGCC crystal  86  in the pumped solid-sate laser  84  according to the present invention. The NIMLGCC crystal  86  can be constructed in a manner as described above and is generally molded and polished to a typical optics standard. In this way, a first wavelength, such as from a 405 nm emitting Indium Gallium Nitride (InGaN) diode  88  of the light source  67 , reflects between the input and output mirrors  78 ,  80  as a coherent emission within laser cavity  75 . At least a portion of this first wavelength can be absorbed by the NIMLGCC crystal  86  and a second wavelength is emitted. This second wavelength will traverse the output mirror  80  and will be emitted as the laser output. 
         [0054]    In yet another embodiment, the NIMLGCC can be used as a luminescence collector  90  for energy conversion, as shown in  FIG. 8 . Therein, the NIMLGCC is molded into a sheet acting as a light tube  92 . As a light tube  92 , the phosphor emissions  94  will be contained as total internal reflections  96 , which are directed toward first and second ends  98 ,  100  of the light tube  92 . Total internal reflection  96  is accomplished by the selection of an NIMLGCC material for the light tube  92  in accordance with Snell&#39;s law and as described previously. Thus, the NIMLGCC material should be selected so as to maximize the total internal reflections  96  from the phosphor emissions  94  while minimizing transmitted light  102 . 
         [0055]    In operation of the light tube  92 , a light source  104  emits a first wavelength incident  106  to the light tube  92 . The first wavelength is absorbed by an inorganic crystalline  42  within the NIMLGCC light tube  92  and remitted at a second wavelength. This second wavelength is transmitted through the light tube  92  by total internal reflection  96  to the first or second ends  98 ,  100  of the light tube  92 . As the second wavelength leaves the light tube  92  at the first or second ends  98 ,  100  as reflected light  108 , the reflected light  108  impacts a photovoltaic cell  110 . The photovoltaic cell  110  collects a substantial portion of the reflected light  108  and converts the reflected light  108  into another energy, such as electrical current. 
         [0056]    The light tube  92  can be constructed with a small edge profile, which enables the use of a relatively small photovoltaic cell  110 . Thus, the first and second ends  98 ,  100  of the light tube  92  are approximately similar in size to the surface area of the photovoltaic cell  110 . This allows for increased likelihood that the reflected light  108  will impact the photovoltaic cell  110 . 
         [0057]    Suitable materials for the photovoltaic cell are known, but can generally include Si, Ge, GaAs, AlAs, InAs, AlP, InP, GaP, ZnSe, or CdSe, or combinations thereof. 
       EXAMPLE 1 
       [0058]    The efficiency of the ELIXIR LED  10  according to the present invention is demonstrated with a computer simulation of a ray tracing diagram, shown in  FIG. 9 . Herein, the ELIXIR LED  10  is constructed as described above with a phosphor radius, r, and equal to 1.9 cm. 
         [0059]    The ray tracing diagram illustrates the various paths the phosphor-emitting photons can take in exiting the ELIXIR LED  10 . Ray  1  exits the ELIXIR LED  10  without encountering any reflections and comprises approximately 35% of the phosphor-emissions. Ray  2  (representing approximately 35% of the phosphor-emission) demonstrates one particular benefit of the ELIXIR LED  10 . Ray  2  is emitted in a direction toward the planar reflector  16 , where substantial emissions loss occurs in a conventional pcLED package design. However, in the ELIXIR LED  10 , the phosphor emission is reflected at the phosphor-air interface  112 . Ray  2  can then exit the ELIXIR LED  10  and may avoid the planar reflector  16  entirely. Ray  3 , comprising approximately 17% of the phosphor-emission, heads directly to the reflector  16  before exiting the ELIXIR LED  10  and never encounters the phosphor-air interface  112 . Ray  4  is transmitted across the phosphor-air interface  112  but avoids the LED source  12  and recrosses the phosphor-air interface  112  before exiting the ELIXIR LED  10 . The transmissions represented by Ray  4  account for approximately 13% of the total phosphor emissions. Finally, Ray  5  is transmitted across the phosphor-air interface  112  and enters the LED source  12  where the highest losses would occur within conventional LED package designs. In the ELIXIR LED  10  constructed with a radius of the phosphor  14 , Ray  5  comprises less than 0.1% of the total phosphor-emission. 
         [0060]    While the invention has been illustrated by a description of various embodiments and while these embodiments have been described in considerable detail, it is not the intention of the applicants to restrict or in any way limit the scope of the appended claims to such detail. Additional advantages and modifications will readily appear to those skilled in the art. Thus, the invention in its broader aspects is therefore not limited to the specific details, representative apparatus and method, and illustrative example shown and described. Accordingly, departures may be made from such details without departing from the spirit or scope of applicants&#39; general inventive concept.