Abstract:
Traditional incandescent and halogen lamps produce a high CRI warm white light with indirect emission patterns at the cost of poor energy efficiency. This new advancement in solid-state lighting enables the production of a new solid-state filament wherein the tungsten filament is replaced with an array of high efficiency LED emitters which combine through an equiangular spiral, or t-spline/TNURCC lightpipe network to produce a single homogeneous blue light source which then pumps a luminescent filament comprised of a phosphor loaded silicone, phosphor loaded polymer, a lanthanide doped fluoro-phosphate glass, glass ceramic tape, quantum dot filled composite, or super-continuum spectrum producing photonic crystalline structure.

Description:
CROSS REFERENCE TO RELATED APPLICATIONS 
     This application claims priority from U.S. Provisional Patent Application Ser. No. 61/031,213, entitled “Solid-state luminescent filament lamps”, filed on 25 Feb. 2008. The benefit under 35 USC §119(e) of the United States provisional application is hereby claimed, and the aforementioned application is hereby incorporated herein by reference. 
    
    
     FEDERALLY SPONSORED RESEARCH 
     Not Applicable 
     SEQUENCE LISTING OR PROGRAM 
     Not Applicable 
     TECHNICAL FIELD OF THE INVENTION 
     The present invention relates generally to LED&#39;s or light emitting diodes. More specifically, the present invention relates to a solid-state filament wherein the tungsten filament is replaced with an array of high efficiency LED emitters which combine through a lightguide injector and then convert wavelength and solid-angle distribution after passing through a luminescent cladding. 
     BACKGROUND OF THE INVENTION 
     As of 2009 GaN LED&#39;s or light emitting diodes can produce blue wavelength light at &gt;55% wall-plug efficiency. 55-65% wall plug efficiency for the die sources refers to the production of 550-650 mW of blue light at a wavelength between 405-489 nm for every watt of electrical power. The problem with blue light emission is that the photopic efficacy spectrum requires a large amount of green light to produce luminous flux and a white spectra requires a continuous power from 380-780 nm where in light in the green-red spectrum is of highest importance in the warm white approximating the spectral distribution of a 2700-3000K planckian radiator. Down converting the blue light to yellow and red produces stokes shift quantum loss which is unavoidable. Phosphors available in the yellow, orange, and red wavelengths also incurs internal quantum efficiencies of typically 70-90%. At an operating temperature of 100 deg C. the phosphors down-convert light less efficiently through a non-radiative process known as thermal quenching. 
     For example the typical wavelength conversion efficiency of a red phosphor at a temperature of 115 deg C. is 78%. When combined with the internal quantum efficiency of the phosphor of at best 90% and the stokes shift conversion loss (78-82%) the typical efficiency of a blue/red conversion is approximately (0.82)*(0.9)*(0.78)=0.574 or 57%. The thermal quenching of the phosphor is most problematic when the phosphor layer is directly deposited to the die structure through an electrophoretic deposition process, or through the heat generated at the chip which reduces the wavelength conversion efficiency of a luminescent ceramic chip placed directly on the blue die emitter itself, or when the phosphor loaded silicone or epoxy surrounds the blue or UV LED emitter in the same cavity. 
     Several solutions have been proposed to reduce the problem of thermal quenching and phosphor scattering, including the placement of a thin layer of phosphor loaded silicone remotely from the LED light source but contained in the same LED cavity, or to introduce a dichroic mirror at the exit of a confocal-parabolic concentrator where the blue light excites the phosphor, and then the green-red light is forward reflected giving the opportunity for the back-reflected blue light to recycle and then re-excite the phosphor. 
     The problem with the remote phosphor methods previously proposed by others is that the layer produces a larger source thereby reducing luminance, and still backscatters light into the high index die emitter due to the unavailability of a suitable high index encapsulant to match the die structure and remotely located phosphor composite. One of the shortcomings of the dichroic mirror approach is that the reflectance and transmission efficiency is highly angle dependent, costly to implement, and not manufacturable at the volumes required for an incandescent light bulb replacement. The problem with the luminescent ceramic chip placed directly on the die emitter is that the wavelength conversion will degrade with temperature as the chip heats up. All of these prior methods have the added shortcoming of only producing light in a 180 deg hemisphere which only fills half of the solid angle of distribution produced by the household vertical filament incandescent lamp. 
     SUMMARY OF THE INVENTION 
     A novel solution is to introduce combinations of source and optical engineering innovations to decouple the blue pump light sources from the wavelength conversion elements, to homogenize and unify the individual blue sources into one source, and to pump a wavelength conversion element which is unaffected entirely by the heat of the emitters thereby producing a 22% improvement in wavelength conversion efficiency at high blue light emitter temperatures. The wavelength conversion can be summarized by a string of multipliers including (stokes shift quantum conversionloss)*(internal quantum efficiency)*(efficiency after thermal quenching). 
     A luminescent glass or glass-ceramic filament can improve efficiency of wavelength conversion in several ways, including the elimination of thermal quenching loss and a reduction in scattering by matching the host medium with the phosphor index of refraction. Many Pb-free glasses are available with refractive index approaching 1.8 to match that of the crystalline host materials and lanthanide dopants. Implementing the luminescent filament wavelength conversion will eliminate the thermal quenching loss producing a wavelength conversion efficiency of (0.82)*(0.9)*(1.0)=0.74. The GaN emitters themselves are relatively unaffected by operation at high junction temperature. Operating the die junctions at higher temperature allows for a reduction in the size and surface area of the thermal dissipation structures to give more room for the guidance and direction of the light through a novel optical lens system. Where space and air-flow permits larger thermal dissipation structures may be implemented. 
     Critical to producing an alternative to the incandescent F-12, A-19, B-10, or G-25 lamp is the efficiency of the light source, and the quality of the indirect light pattern produced through the optical system. Much of the LED lamp prior art will bundle together various components comprising a lamp including the heatsink, optical feedback control system to maintain consistent color temperature over time, communication and dimming circuitry and protocols, or LED packaging, but will largely ignore the intricacy of the optical design required to match the intensity distribution of the existing incandescent filament lamp. 
     Other optical designs may produce a combination direct/indirect beam pattern but only work with a single 1 Watt LED emitter. Detailed optical simulation models and measurements of common filament lamps were conducted to produce a proper optical merit function for the design of the next generation solid state lamp. Critical to its novelty is the unification of light wavelength conversion with optical lens design to produce hybrid direct/indirect intensity distribution of light pleasing to the eye. 
    
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
       The accompanying drawings, which are incorporated herein and form a part of the specification, illustrate the present invention and, together with the description, further serve to explain the principles of the invention and to enable a person skilled in the pertinent art to make and use the invention. 
         FIG. 1   a . illustrates an incandescent light bulb from IESNA lighting handbook Ver.9; 
         FIG. 1   b . illustrates an incandescent light bulb filament structure and shape; 
         FIG. 1   c . illustrates a flame or candelabra incandescent light bulb; 
         FIG. 1   d . illustrates a bulb tungsten filament structure and geometry; 
         FIG. 1   e . illustrates a lamp; 
         FIG. 1   f . illustrates a tungsten filament structure and geometry; 
         FIG. 1   g . illustrates various incandescent filament geometries; 
         FIG. 2   a . illustrates a raytrace and optical model of a typical vertical filament A-19 lamp; 
         FIG. 2   b . illustrates a lamp source model modeled including lamp structure and correct material properties; 
         FIG. 2   c . illustrates an intensity distribution of the vertical filament lamp of  FIG. 2   a  and  FIG. 2   b;    
         FIG. 3   a . illustrates a wavelength conversion material directly deposited on LED emitter; 
         FIG. 3   b . illustrates a wavelength conversion chip directly bonded to the active emission structure of the LED; 
         FIG. 3   c . illustrates a light source wavelength conversion performance; 
         FIG. 4 . illustrates a delectric/air interface losses of typical snap-on secondary optics; 
         FIG. 5 . illustrates a next generation solid-state luminescent glass filament lamp; 
         FIG. 6 . illustrates luminescent filament detail1 with single trunk lightguide; 
         FIG. 7 . illustrates a raytrace of a luminescent filament; 
         FIG. 8 . illustrates a the globe of light produced through a solid-state luminescent filament system; 
         FIG. 9 . illustrates a solid-state emitter coupled to a TIR lightguide; 
         FIG. 10 . illustrates an intensity pattern of the luminescent filament structure described in  FIG. 7 ; 
         FIG. 11 . illustrates a figure representing a “FlexFilament” approach to lamp design; 
         FIG. 12 . illustrates a light raytrace of the luminescent filament shown in  FIG. 11 ; 
         FIG. 13 . illustrates an intensity distribution of the “Flexfilament” design1 of  FIG. 12 ; 
         FIG. 14 . illustrates a flexfilament design; 
         FIG. 15 . illustrates a resulting intensity distribution as produced by the luminescent filament geometry depicted in  FIG. 14 ; 
         FIG. 16 . illustrates an asymmetric design luminescent flex filament; 
         FIG. 17 . illustrates an asymmetric flex filament luminescent filament; 
         FIG. 18 . illustrates a perspective view of the flex filament design; 
         FIG. 19 . illustrates a luminescent flex-filament design; 
         FIG. 20 . illustrates a luminescent flex-filament design; 
         FIG. 21 . illustrates a G-25 lamp incorporating the flex-filament optical system; 
         FIG. 22 . illustrates a perspective view of the luminescent filament system incorporated into a G-25 lamp; 
         FIG. 23 . illustrates a light emission cavity array comprised of 4 cavities with 1 emitter each; 
         FIG. 24 . illustrates a 4-cavity array in a triangular pattern with a central cavity; 
         FIG. 25 . illustrates a light emission cavity pattern comprised of 6 cavities in a star arrangement; 
         FIG. 26 . illustrates a 7-cavity Light emission cavity array to pump the luminescent filament; 
         FIG. 27 . illustrates a 5-cavity light engine array; 
         FIG. 28 . illustrates a single light emission cavity with large solid state light producing device; 
         FIG. 29 . illustrates a square single cavity with 4 die emitters; 
         FIG. 30 . illustrates a larger single light emission cavity with 16 emitters; 
         FIG. 31 . illustrates an intensity distribution of typical light emitting diode; and 
         FIG. 32 . illustrates a super-gaussian intensity distribution provided by photonic crystalline structures on light emitter. 
     
    
    
     DETAILED DESCRIPTION OF THE INVENTION 
     In the following detailed description of the invention of exemplary embodiments of the invention, reference is made to the accompanying drawings (where like numbers represent like elements), which form a part hereof, and in which is shown by way of illustration specific exemplary embodiments in which the invention may be practiced. These embodiments are described in sufficient detail to enable those skilled in the art to practice the invention, but other embodiments may be utilized and logical, mechanical, electrical, and other changes may be made without departing from the scope of the present invention. The following detailed description is, therefore, not to be taken in a limiting sense, and the scope of the present invention is defined only by the appended claims. 
     In the following description, numerous specific details are set forth to provide a thorough understanding of the invention. However, it is understood that the invention may be practiced without these specific details. In other instances, well-known structures and techniques known to one of ordinary skill in the art have not been shown in detail in order not to obscure the invention. 
     Referring to the figures, it is possible to see the various major elements constituting the apparatus of the present invention.  FIG. 1  illustrates an known Incandescent light bulb  18  as taught in the IESNA Lighting handbook Ver.9. A Tungsten filament  11   n  precise ring shape and position relative to a glass envelope shape  12 . Other filament structures commonly found include a vertical coiled coil and horizontal coiled coil. The glass envelope of precise optical shape  12  is internally filled with argon to reduce tungsten deposit on the inside of the glass envelope shape  12 . A Molybdenum support, glass button, exhaust hole  13  and an arbor tube and exhaust tube  14  are connected to an E26 base and contact  15  to complete the device. 
     The incandescent light bulb filament structure and shape  11  is shown in  FIG. 1   b . The Tungsten filament structure  11  is comprised of a ring with specific diameter, coil pitch, and approximately two meters in length, alignment of filament shape to the glass bulb geometry is critical to 3d intensity lobe shape. Luminance of the source is approximately 1.2 E5 cd/m^2. 
     Now referring to  FIGS. 1   c  and  1   d , a flame or candelabra Incandescent light bulb  17  is shown. A Tungsten filament with a peak or tent-like shape  16  with specific coil diameter, pitch, and position relative to the glass envelope  12  is shown. A Tungsten filament with a tent-like structure produces a flame intensity pattern matched to the glass envelop geometry. For the glass envelope  12  to shape light, the shield filament structure contains argon fill that prevents tungsten build up on the inside of the glass. The flame or candelabra Incandescent light bulb  17  is also comprised of an arbor, exhaust tube, glass button  13 , and Arbor tube and stem  14 , and E12 base and contacts  15 . 
       FIG. 1   e  and  1   f  illustrate a G-25 lamp  19 , which is comprised of a Tungsten filament with two or three spans with specific coil radius, pitch, and shape  20 , a globe glass envelope  22 , a glass arbor, exhaust tube, contact wires  13 , and an E26 medium base with contact  21 . 
     Primarily the filament geometries C-9, C-6, C-7A, C-8, C-2V, and C-11, and C-11V, shown in  FIG. 1   g ., have found the most use in incandescent bulbs used in residential lighting fixtures. The CC-6 coil is a correct representation of the fine structure of the filament in which a helical filament is then itself coiled into a global super helical structure. Many of the C-9, C-6, C-8, C-7A, C-2V could be designated CC for “Coiled Coil”. This coiled coil structure further boosts luminous efficacy. The figure is included to illustrate the fine design details required to produce even a low luminous efficacy source. 
       FIG. 2   a  illustrates a raytrace and optical model of a typical vertical filament A-19 lamp. The light  21  produced from the vertical tungsten filament passes through the glass envelope to the outside. Some rays  22  within the 140-170 deg half angle zone do not pass through the glass envelope due to fresnel reflection. The illuminance distribution is portrayed on a detector screen positioned in close proximity to the lamp source. 
       FIG. 2   b . illustrates an A-19 lamp source model modeled including lamp structure and correct material properties. The glass envelope  25  shown in this figure is tailored to the emission shape of light distribution as it emerges from the filament structure. Ideally the fresnel losses are kept to a minimum to allow light to exit without back reflection or tunneling of the light into the wall of the glass envelope. Reduced fresnel back reflection occurs by maintaining near normal ray incidence with the dielectric/air interface. 
       FIG. 2   c . illustrates the intensity distribution  26  of the vertical filament A-19 lamp of  FIG. 2   a  and  FIG. 2   b . A typical filament-based bulb such as A-19, F-12, or G-25 and the similar sub-classes produce a combination direct/indirect intensity distribution in which the full-width at the field angle in which the field angle constitutes the angular dispersion at which the intensity falls off to 10% of the peak is typically 240, 280, or 300 deg full angle. Depicted in  FIG. 2   c  is one half of the full intensity distribution depicting the fall-off of intensity with angular deviation from the axis directly above the bulb constituting the zero-degree reference. 
     Now referring to  FIG. 3   a ., wavelength conversion of material directly deposited on LED emitter  31  is shown. The LED emitter structure  31  in which the wavelength conversion layer  32  is deposited directly to the active emission structure of the device is shown. The wavelength conversion material and layer  32  operates near the temperature of the LED emitter producing inefficient conversion due to thermal quenching. Lifetime of the LED as well as white point consistency over time suffers. 
     A wavelength conversion chip  33  can be directly bonded to an active emission structure  33  of the LED semiconductor or the back of the substrate material in the case of a flip-chip emitter.  FIG. 3   b  shows a solid-state pump device or LED  35 , where a wavelength conversion chip  33  is comprised of a luminescent ceramic tape. The luminescent ceramic performs less efficiently at high temperature, and scatters light directly into the absorbing active structure of the LED emitter  34 . Some of the light is re-emitted through photon recycling but most is absorbed and lost. As shown in  FIG. 3   c  typical blue LED&#39;s perform between 90-96% of radiometric power level as compared to operation at 25 deg C. Yellow-Red phosphors perform at 75% at typical operating temperatures due to thermal quenching. 
       FIG. 4  depicts a traditional LED package  40  in which the LED emitters are immersed in a silicone with a snap-on light redirection device. Light will trap and back reflect at the glass, silicone, or plastic hemisphere/air interface due to total internal reflection  41 . Light is also back reflected and lost at the air/lens interface  42 . An additional 4% of the light is lost due to internal back reflections at the exit lens/air interface  43 . It is difficult to design secondary optics which are better than 88% efficient due to these three interface ray splitting losses. It would be advantageous to eliminate at least two of these three interfaces. 
       FIG. 5  depicts a solid state luminescent filament replacement for the A-19 tungsten filament bulb which has gained such prevalence over many decades. The next-generation lamp consists of a system of novel optical design elements including a b-spline, polynomial, t-spline, T-NURCC, NURBS, or NSS described combination source filament comprised of a luminescent glass such as but not limited to a fluoro-phosphate or oxy-sulphide halide glass doped with rare earths optimally combined to produce a high CRI preferably 80+ and a color temperature of 2700-3000K. The filament structure serves a dual purpose, both to convert light and to direct the light in such a manner that it matches the emission intensity profile of the tungsten A-19 lamp or G-25. 
     The filament structure is not limited to glass, or glass/ceramic. The filament structure may also be comprised of a loaded polymer and the wavelength conversion may also be performed through a photonic crystalline structure. Photonic crystalline structures have produced narrow to wide-spectrum behavior through strong non-linearity as used in optical coherence tomography in which the source is an ultra wide-band supercontinuum spectrum. 
     Such photonic crystalline wavelength conversion structures may be designed through the aid of an evolutionary optimization tool. The material of the wavelength conversion light redirection device would ideally match the wavelength conversion mechanism in the case of a rare-earth loaded polymer or glass to reduce back scattering to a minimum. 
     The wavelength conversion shell  51  as shown may also be described in terms of a “cladding”. In which the filament structure comprised a minimum of three parts: The wavelength conversion shell  51  whose shape is specifically tailored to redirect light to match that of a indirect/direct source, the inner structure  52  is structured in thickness to maximize light transfer efficiency, wavelength conversion efficiency free from thermal quenching, and to maintain constant color temperature in the beam intensity zones as desired. The inner “core”  53  where the blue light emerges from the high efficiency lightguides tunnels, frustrates TIR and passes through the wavelength conversion shell before redirection. A lightpipe network  54  is comprised of high efficiency, low absorption glass, polymer, or photonic crystalline holey fiber structure. The waveguide must combine light from a spider of source locations, or direct and guide through high efficiency TIR the light from a central lightpipe trunk illuminated by a large emitter or emitter array capable of producing 4-5 Watts of UV-Blue light. The geometry of the lightpipe combiner  54  in which equiangular spirals are most efficient, but extended free-form t-splines, b-spline NURBS or NSS surfaces are also powerful computational geometry tools with which to combine and direct light to the central luminescent filament section. 
     The thermal dissipation structures  56  are required for such a lamp in which the structures may be designed through the aid of evolutionary algorithms. The thermal dissipation structures are commonly comprised of Aluminum, or Copper. Thermal dissipation required attention to detail from the Multiple-quantum wells out to the air. Structures which work well include Copper substrate die emitters, eutectic die attach, elimination of a metal core board with direct attachment to an isolated or printed heatsink interface, etc. The thermal dissipation fins should be spaced, positioned, and shaped in such a manner that junction temperatures do not exceed 100 deg C. The thermal dissipation structure may be painted black to improve radiative transfer or textured. 
     The lamp of the present invention requires a power electronics device  57  to convert line AC to stabilized power factor corrected DC to drive the solid-state emitter devices. The power electronic components may be arranged and designed through the aid of an evolutionary computational tool in which topology search algorithms enhanced through genetic, harmonization, or other gene expression behaviour in biology enhance the speed of global geometry discovery. In a localized case the design tools aid the selection, arrangement, and design layout. It is desired that the power transfer from line to light engine device is &gt;99% efficient to within the spacing limitations of the lamp. Optical feedback control means may also be integrated to the power electronics cluster to avoid thermal over heating, or to tune wavelength emitters to a desired color temperature. Such optical control circuits may be designed through an evolutionary optimization tool and enhanced through neural network design methodology. 
     The E26 base  58 , although a bi-pin base or next generation solid-state base is also possible. The envelope structure  59  is ideally tailored to reduce fresnel reflections. The envelope structure  59  may be blow molded from hard silicone, glass, or other polymers. The protective envelope structure may also contain moth eye nano-structure to drastically reduce fresnel losses at both the incident and exit surfaces. The glass or other material envelope may also be comprised of an active material as well in which “active” refers to wavelength conversion or light redirection. The extended free-form structure may be comprised ideally from T-spline geometry, T-NURCC or D-NURBS to locally design geometry which optimizes orthogonal interfacing for each ray bundle directional class. 
       FIG. 6 . illustrates the luminescent filament light redirection shape  61  used to produce an indirect/direct light intensity pattern. The luminescent filament structure wall or “cladding” 62  surrounds the tapered pump “core”  63  in which frustrated TIR UV-Blue light pumps a wavelength conversion shell which itself specifically tailored to optically control light distribution. A lightpipe section  64  directs light to the luminescent filament structure. The collimation device  65  is directly coupled to the solid-state emitter or emitter array. The package  66  which encloses the emitters in which a high index encapsulant such as silicone improve external quantum efficiency. The silicone itself may be loaded with higher index nano-particles such as ZrO2, or Tantalum Pentoxide to further extract light from the emitter. The emitters may be nano-roughened or patterned with photonic crystalline structure to improve light transfer efficiency from the light emission section to the integral or monolithic lightguide. 
       FIG. 7  depicts the ray tracing of the luminescent filament  71  in which ray tracing refers to the evaluation through optical physics software the active computational geometry comprising the luminescent filament structure. The luminescent structure loaded with rare-earths directs ray-paths according to the mean free-path and cross section of the particles with respect to the bulk material. An efficient TIR lightguide or holey photonic band-gap lightguide directs light from the light emission center to the wavelength conversion and optical direction device. 
     The globe of light produced through a solid-state luminescent filament system is shown in  FIG. 8 . The ray bundles  81  emerge from the luminescent filament structure. As shown a combination of direct and indirect light mimics the light emission pattern produced by a tungsten filament lamp. 
       FIG. 9  describes the solid-state emitter package  92  coupled to a TIR lightguide  91  comprised of glass or other materials with high visible transparency. A combination of direct and indirect light verifies the operation of the luminescent filament optical structure as shown in  FIG. 10   
       FIG. 11  represents a “FlexFilament” approach to lamp design. As shown in  FIG. 11 , t a 40% shorter luminescent filament  111  with a slightly different light redirection spline geometry is shown. The introduction of alternative luminescent filament designs allows for the production of many source lamps with custom light intensity distributions for style and aesthetic lighting design purposes. 
       FIG. 12  illustrates the light raytrace of the luminescent filament  111  shown in  FIG. 11 . As shown in  FIG. 13  the light distribution pattern now produces more direct light than the intensity pattern of  FIG. 10 . Lighting fixtures vary in their requirements and as such adjustments to the filament structure may change as required. 
       FIG. 14  describes a luminescent filament design which closely matches that of a vertical filament A-19 intensity distribution. The geometry shown includes only one central lightpipe trunk  141 , and is a representation only. The central lightpipe trunk  141  may be replaced with a high efficiency lightpipe spider network in which the lightpipe channels are comprised of T-splines or extended free-form geometry or equiangular spiral described lightpipe sections which combine multiple cavities of light emitters. 
       FIG. 15  illustrates the resulting intensity distribution as produced by the luminescent filament geometry depicted in  FIG. 14 . The intensity pattern shown describes the light intensity as produced by the luminescent filament depicted in  FIG. 14 . The light distribution has zero degree directly below the light array source in which no light emerges through the thermal dissipation structures and the majority of the light passes to the side with a slight reduction in relative intensity at the 180 degrees intensity zone directly above the light source. 
       FIG. 16  shows a luminescent flex filament with an asymmetric design. Here the ZX cross section of a luminescent filament  161  design in which the cross-sections are asymmetric produces a fan-shaped intensity distribution.  FIG. 17  shows an asymmetric luminescent filament. The ZY cross section of the luminescent filament  171  design in which the cross-sections are asymmetric to produce a fan-shaped intensity distribution. 
       FIG. 18  illustrates a flex filament. The Flex filament  181  in which the luminescent filament structure is asymmetric produces an intensity distribution that is wider in one cross section than the other. 
       FIG. 19  discloses a luminescent flex-filament teaching a luminescent filament ring structure  191  to mimic the incandescent light source of  FIG. 1   a.    
       FIG. 20  discloses a luminescent flex-filament  201  in which the design structure produces an indirect/direct ring of light to mimic the light distribution pattern produced by a ring tungsten filament lamp. 
       FIG. 21  discloses a G-25 lamp incorporating the flex-filament optical system.  FIG. 21  is a depiction of the elements necessary for a next generation G-25 lamp based upon luminescent filament structure, high efficiency extended free-form lightpipes to combine and pre-process light fields before entering the wavelength conversion section and beam shaping surfaces. The outer protective envelope  211  may be manufactured from glass, optical grade polymers or silicones. The material shape may be comprised of extended free-form t-spline geometry preferably, or D-NURBS, and may be optically inactive serving only to protect the interior optical system components. When optically passive the envelopes three dimensional shape ideally produces local surface normals with respect to the incident light fields to reduce fresnel reflection losses at the interface. Surface texturing may be applied to produce a diffuse source with reduced glare and luminance as a transfer of light emission from the luminescent filament to the outer envelope structure. Scattering however is detrimental to light transfer efficiency. 
     The outer envelope  211  may also be comprised of active glass, polymer, or silicone in which the active material performs wavelength conversion or redirection. In the figure the outer envelope thickness is constant but through controlled variable thickness light beam control may be performed by the outer envelope as well. If serving only a passive function the outer envelope may comprise nano-structure such as moth-eye trees of wavelength scale to enhance anti-reflection properties and overall efficiency. Item 2 refers to the luminescent filament structure. 
     The luminescent filament structure  212  is comprised of either a phosphor loaded glass, glass-ceramic, or active polymer. Photonic crystalline structures may also perform wavelength conversion through the supercontinuum effect. Photonic-crystalline structures may also guide and direct light on the interior of the luminescent filament. The cladding of the luminescent filament in this embodiment constitutes the wavelength converter in which UV-Blue light is down converted to white light comprised of Green, Yellow, and Red. The luminescent filament structure  212  in this embodiment has five faces forming a tapered pentagon structure to further direct the light emission. The light emission “cladding” also has a tailored outer wall at the air or inert gas interface. The cladding shape serves to homogenize white light color temperature within the beam emission and to form the combination of indirect/direct light required to match the incandescent beam emission pattern of  FIG. 2   c . As such the novel luminescent filament structure  212  performs a dual purpose in that it converts wavelength and shapes light emission. The light received from the tapered “core” serves to pump the active cladding. Tapering angles are balanced to provide sufficient light field frustrated TIR properties as well as uniform pump excitation of the active cladding. 
     The lightpipe coupler region  213  transfers UV-Blue light from the combiner to the luminescent filament structure  212 . A lightpipe field shaping device  214  in which light exiting the spider lightpipe network is converted from a rectangular illumination field to a circular or rotationally symmetric shape before transfer into the luminescent filament. The lightpipe shaping device  214  may be comprised of high transparency glass, polymer, or photonic band-gap cores or bundles. The lightpipe shaping device  214  may incorporate faceting features or ridges to further homogenize light. 
     The lightpipe combining section  215  directs light from the light emission cavities through the operation total internal reflection. Extended free-form t-splines, NURBS, or variations on the equiangular spiral are most efficient at directing the transfer of light with minimal loss. The thermal dissipation structures  216  channel heat from the LED or other solid state emitters to air. The thermal dissipation structures  216  are typically comprised of forged or cast aluminum or copper or other low thermal resistance alloys. The shape can be optimized using evolutionary algorithms to derive the appropriate structure to direct heat away and dissipate to the air in which natural convection dominates. The thermal dissipation structures may be painted black or textured and tapered depending on the flow fields. The glass envelope  211  may also give way to more thermal dissipation structures  216  at the cost of less indirect light and a comprise must be achieved in the interest of achieving the highest optical performance and beam pattern shaping. 
     The E26 base  217  retains a power electronics device, dimming circuit, and optical feedback control devices incorporated in the interior cavity. The power electronics devices producing the most heat may also be directly coupled to the thermal dissipation structures for the light generation engine. 
       FIG. 22  is a perspective view of the luminescent filament system incorporated into a G-25 lamp. An envelope protection or active structure encloses a luminescent filament  222  comprised of five facets an active “cladding” and a tapered core; a lightpipe to filament combiner  223 ; a lightpipe transfer confocal elliptic concentrator  224  although the ellipse may be replaced by an extended free-form t-spline, T-NURCC, or D-NURBS structure; a lightpipe combiner  225  which pulls light from the light engine cavity arrangement to the transfer geometry; thermal dissipation structures  226  to channel heat away from the light engine and power electronics to the air; and an E26 base  227  which contacts to an Edison socket to provide power to the solid-state lamp. The glass envelope  221  may be tailored to allow for free-airflow through the dissipation structures as required. Power electronics, dimming circuitry, communication devices, or optical feedback control systems may be incorporated on the inside cavity of the contact base  227 . 
       FIG. 23  illustrates a light emission cavity array comprised of four cavities with one emitter each. Four light emission cavities  231 ,  232 ,  233 , and  234  are arranged in a square or rectangular arrangement in a 2×2 arrangement although a linear 1×4 arrangement is also an alternative. Separation of the cavities serves to spread the heat sources out for better channeling to the thermal dissipation devices. More than one light emitter  235  may be placed in each cavity. The light emitter  235  may be a light emission device GaN UV-Blue, ZnO emitter, laser diode, or resonant-cavity LED. The light emitter  235  is secured to a substrate  236  upon which the light emitter  235  is attached preferably through a eutectic attachment material. The emission cavities  231 ,  232 ,  233 , and  234  may be comprised of an overmolded lead frame composed of a highly reflective plastic, or a ceramic layered structure, or other glass filled composites. 
       FIG. 24  illustrates a four-cavity array in a triangular pattern with a central cavity  241 . The light emission cavities comprise a triangular arrangement with a central light emission cavity  241 . More than one light emitter  242  per cavity is also possible. The light emission cavities  241 ,  243 ,  244 ,  245  serve to supply power to the UV-Blue LED&#39;s, to encapsulate the emitters  242 ,  246 ,  247 ,  248  with silicone, or direct contact glass, in which a micro-particle loaded silicone or glass better extract light from the high index GaN or ZnO emitters. Blue light is not a limitation. UV-IR light emission devices may also be incorporated with combinations of direct emission and low stokes shift loss wavelength conversion. For example to boost CRI in the 2850K a direct emission red emitter may be incorporated in one of the cavities, or a blue may be converted to a red through nitride based phosphor applied directly to the blue or UV emitter, but preferably the wavelength conversion will occur in the luminescent filament section to eliminate thermal quenching. 
       FIG. 25  illustrates a light emission cavity pattern comprised of six cavities in a star arrangement  250 . The light emission cavities comprising this star arrangement may contain 1 to 12 light emitters each. The die structure themselves are preferably Copper substrate emitters in which the active structures are grown on GaN, Sapphire, or ZnO, then through a laser lift-off procedure taken away then bonded directly to a Cu substrate. This greatly enhanced thermal conduction from the active layer to the metal-core board, AlN interposer, or directly attached to the patterned and isolated thermal dissipation device preferably comprised of Cu or Al or other highly conductive alloy. 
       FIG. 26  illustrates a seven-cavity light emission cavity array  260  to pump the luminescent filament. The seven-cavity array of light emitting diodes, lasers, resonant cavity light emitters, or photonic crystal patterned amplified spontaneous emission devices. The light emission devices may be attached to a BeO, AlN, Cu, CuMo, or CuW, Al, or other substrate through InS, AuS, or CVD diamond attach material. Microchannels may be incorporated under the thermal dissipation device for air flow, water flow, or for heat piping in which a heat pipe transfers light from the heat source centers to the thermal dissipation devices cooling through radiation and natural convection. 
       FIG. 27  illustrates a five-cavity light engine array  270 . A five-cavity light emission array serves to apply power to the light emitting junction device, to extract light through encapsulation or direct glass attachment, and to protect the LED&#39;s. 
       FIG. 28  illustrates a single light emission cavity  280  with large solid state light producing device  281 . In this figure the light emission cavity is larger and contains a large light emitting diode  282  which may be up to 16 mm^2 in area. Vertical structure light emitters are preferred as they can produce light efficiently at larger cross-sectional area. The light emitting diode  282  may be either Cu substrate based or flip-chip in which the active structure is closest to the thermal dissipation structures allowing for more intimate contact of the lightpipe sections to the light emission device thereby reducing the cross-sectional area of the lightpipe required to capture and redirect the light through the operation of TIR waveguiding. 
       FIG. 29  illustrates a square single cavity  290  with four die emitters  291 ,  292 ,  293 ,  294 . In this embodiment the die emitters  291 ,  292 ,  293 ,  294  are placed close together to increase luminance in a single square cavity  290 . The cavities may be filled with high index silicone or Sol-gel to extract light from the high index GaN, InGaN, and AlInGaN layers. AlGaInP emitters especially benefit from high index encapsulation to boost external quantum efficiency. The cavity structure  295  may be comprised of polythalamide or LCP a liquid crystal filled polymer. 
       FIG. 30  illustrates a larger single light emission cavity  300  with sixteen emitters  301 . A large single light emission cavity  300  filled with sixteen individual smaller emitters  301  which may be each 0.3-4 mm^2 in area. Vertical structure junctions are critical with close light emission packing. The sixteen emitters  301  also preferably are Cu substrate emitters or flip-chip structure. The interposer or sub-mount  303  is preferably comprised of Cu, AlN, Al, CuMo, or CuW. 
       FIG. 31  illustrates the intensity distribution of typical light emitting diode. A typical light emitting diode produces a lambertian intensity distribution. The equation shown in Table 1 describes the light fall off with angle with S factor=3. These light emitters source the lightpipes, which feed the luminescent filament or filaments. The disadvantage of a lambertian intensity emission is the required area to collimate and direct the light through TIR. 
     
       
         
               
             
           
               
                 TABLE 1 
               
               
                   
               
             
             
               
                 
                   
                     
                       
                         
                           
                             I 
                             ⁢ 
                             
                               { 
                               r 
                               } 
                             
                           
                           = 
                           
                             
                               I 
                               0 
                             
                             ⁢ 
                             
                                 
                             
                             ⁢ 
                             exp 
                             ⁢ 
                             
                               { 
                               
                                 
                                   - 
                                   2 
                                 
                                 ⁢ 
                                 
                                   
                                     ( 
                                     
                                       r 
                                       
                                         w 
                                         S 
                                       
                                     
                                     ) 
                                   
                                   S 
                                 
                               
                               } 
                             
                           
                         
                         , 
                       
                     
                   
                 
               
               
                   
               
               
                 
                   
                             
                     
                         
                         
                     
                   
                 
               
               
                   
               
             
          
         
       
     
     Now referring to  FIG. 32 , a super-gaussian intensity distribution provided by photonic crystalline structures on light emitter is shown. The light emission profile shown in  FIG. 31  is a super-gaussian intensity profile which provides for more uniform excitation of a luminescent ceramic chip, or for higher efficiency coupling to a lightguide. Lightguides when imperfectly manufactured contain micro-roughness which slightly degrades the operation of TIR over length reducing light transfer efficiency. It is highly advantageous to guide the light from the light emission devices with an efficiency greater than the thermal quenching loss which would have occurred with direct application of the wavelength conversion mechanisms. The light guidance devices should provide higher than 85% efficiency to produce an advantage. Glasses and polymers with internal transmittance higher than 98% are readily available. The super-gaussian beams described are used in the laser industry to pump active thin disk materials or second harmonic generation producing non-linear crystals. 
     The light emission structure of the quantum well layers is coupled to a photonic crystalline device which shapes the light emission profiles at high efficiency. Careful attention must be paid to reducing defects through HVPE growth on GaN, non-polar sapphire, or through exciton center isolation nano-pillars. Patterned substrates help induce ideal mode energy profiles, as do combinations of photonic-crystalline structure with nano-roughening on the top surface or nano-roughening of the cleaved edges. 
     
       
         
               
             
           
               
                 TABLE 2 
               
               
                   
               
             
             
               
                 
                   
                     
                       
                         
                           
                             I 
                             ⁢ 
                             
                               { 
                               r 
                               } 
                             
                           
                           = 
                           
                             
                               I 
                               0 
                             
                             ⁢ 
                             
                                 
                             
                             ⁢ 
                             exp 
                             ⁢ 
                             
                               { 
                               
                                 
                                   - 
                                   2 
                                 
                                 ⁢ 
                                 
                                   
                                     ( 
                                     
                                       r 
                                       
                                         w 
                                         S 
                                       
                                     
                                     ) 
                                   
                                   S 
                                 
                               
                               } 
                             
                           
                         
                         , 
                       
                     
                   
                 
               
               
                   
               
               
                 
                   
                             
                     
                         
                         
                     
                   
                 
               
               
                   
               
             
          
         
       
     
     Ideally &gt;99% of the light should emit from the top surface with a super-gaussian light emission intensity distribution constituting an S value &gt;12. An S value equal to fifteen is shown in Table 2. The half beam angular dispersion is also reduced from 50 degrees in  FIG. 30 to 35  degrees in  FIG. 31 . This can enhance light transfer efficiency by 3-7% when using imperfect lightguiding structures to pull light from the light emission cavities to the luminescent filament device. 
     Furthermore, other areas of art may benefit from this method and adjustments to the design are anticipated. Thus, the scope of the invention should be determined by the appended claims and their legal equivalents, rather than by the examples given.