Automotive Solid-State Retrofit Headlamp

Abstract

In an embodiment an automotive solid-state headlamp includes a lamp body extending in a longitudinal direction, the lamp body having a rear base portion and a front portion and including a support member disposed in a light-transmissive housing, a plurality of solid-state light sources arranged on the support member at the rear base portion of the lamp body, and a drive circuitry electrically coupled to the light sources and arranged at the rear base portion of the lamp body and configured to operate the plurality of light sources when energized, wherein the plurality of light sources, when energized, are configured to cause the solid-state lamp to emit, through the light-transmissive housing (a) a luminous flux of at least 1500 lumens +/−10% when energized with a 13.2 Volt test voltage, or of at least 1750 lumens +/−10% when energized with a 28 Volt test voltage, or (b) a luminous flux of at least 1350 lumens +/−10% when energized with a 13.2 Volt test voltage, or of at least 1600 lumens +/−10% when energized with a 28 Volt test voltage.

Claims

1.-32. (canceled)

33. An automotive solid-state headlamp comprising: a lamp body extending in a longitudinal direction, the lamp body having a rear base portion and a front portion and including a support member disposed in a light-transmissive housing; a plurality of solid-state light sources arranged on the support member at the rear base portion of the lamp body; and a drive circuitry electrically coupled to the light sources and arranged at the rear base portion of the lamp body and configured to operate the plurality of light sources when energized, wherein the plurality of light sources, when energized, are configured to cause the solid-state lamp to emit, through the light-transmissive housing: (a) a luminous flux of at least 1500 lumens +/−10% when energized with a 13.2 Volt test voltage, or of at least 1750 lumens +/−10% when energized with a 28 Volt test voltage, wherein the lamp spatially is not in excess of an envelope according to FIG. 2 on page 35 of Addendum 36 of ECE Regulation 37 (3 Jul. 2012) for an H7-type lamp, or (b) a luminous flux of at least 1350 lumens +/−10% when energized with a 13.2 Volt test voltage, or of at least 1600 lumens +/−10% when energized with a 28 Volt test voltage, wherein the lamp spatially is not in excess of an envelope according to FIG. 2 on page 50 of Addendum 36 of ECE Regulation 37 (3 Jul. 2012) for an H11-type lamp.

34. The automotive solid-state headlamp of claim 33, wherein the plurality of light sources, when energized, are configured to cause the solid-state lamp to emit, through the light-transmissive housing a luminous flux of at least 1500 lumens +/−10% when energized with a 13.2 Volt test voltage, or of at least 1750 lumens +/−10% when energized with a 28 Volt test voltage.

35. The automotive solid-state headlamp of claim 33, wherein the plurality of light sources, when energized, are configured to cause the solid-state lamp to emit, through the light-transmissive housing a luminous flux of at least 1350 lumens +/−10% when energized with a 13.2 Volt test voltage, or of at least 1600 lumens +/−10% when energized with a 28 Volt test voltage.

36. The automotive solid-state headlamp of claim 33, wherein, when the plurality of light sources is energized, a radiation pattern of the light emitted through the light-transmissive housing is generated in a plane defined by a longitudinal axis and an axis in a reference plane orthogonal to the longitudinal axis, and wherein an angle of radiation emitted at a luminous intensity amounting to at least half of a maximum luminous intensity in the plane is at least 40 degrees.

37. The automotive solid-state headlamp of claim 36, wherein the angle of radiation emitted in the plane at a luminous intensity which is at least half of a maximum luminous intensity is at least 50 degrees.

38. The automotive solid-state headlamp of claim 36, wherein the angle of radiation emitted in the plane at a luminous intensity which is at least half of a maximum luminous intensity is at least 60 degrees.

39. The automotive solid-state headlamp of claim 33, wherein, when the plurality of light sources is energized, a radiation pattern of the light emitted through the light-transmissive housing is approximately rotationally symmetric about the longitudinal direction.

40. The automotive solid-state headlamp of claim 33, wherein, when the plurality of light sources is energized, a light emitting efficiency of light emitted through the light-transmissive housing per electrical power input to the drive circuitry is at least 100 lumens per watt.

41. The automotive solid-state headlamp of claim 40, wherein, when the plurality of light sources is energized, the light emitting efficiency of light emitted through the light-transmissive housing per electrical power input to the drive circuitry is at least 120 lumens per watt.

42. The automotive solid-state headlamp of claim 40, wherein, when the plurality of light sources is energized, the light emitting efficiency of light emitted through the light-transmissive housing per electrical power input to the drive circuitry is at least 150 lumens per watt.

43. The automotive solid-state headlamp of claim 33, wherein a factor k1, substantially expressing a relative amount of UV-A radiation power with respect to a luminous flux of visible light emitted through the light-transmissive housing, is defined as: $k1=\frac{\begin{array}{c}\lambda =400\mathrm{nm}\\ \int \mathrm{Ee}\left(\lambda \right).Math.d\lambda \\ \lambda =315\mathrm{nm}\end{array}}{\begin{array}{c}\lambda =780\mathrm{nm}\\ k_m.Math.\int \mathrm{Ee}\left(\lambda \right).Math.V\left(\lambda \right).Math.d\lambda \\ \lambda =380\mathrm{nm}\end{array}}\mathrm{is}\le 2.Math.{10}^{-4}W/\mathrm{lm}$ wherein: Ee (λ) as measured in W/nm is a spectral distribution of a radiant flux, V (λ) is a dimensionless spectral luminous efficiency, k.sub.m provided as 683 lm/W is a photometric radiation equivalent, and λ as measured in nm is a wavelength, and wherein value k1 is calculated using intervals of the wavelength λ of five nanometers.

44. The automotive solid-state headlamp of claim 43, wherein the factor k1 is ≤2.Math.10.sup.−5 W/lm.

45. The automotive solid-state headlamp of claim 33, wherein a factor k2, substantially expressing a relative amount of UV-B radiation power with respect to a luminous flux of visible light emitted through the light-transmissive housing, is defined as: $k2=\frac{\begin{array}{c}\lambda =315\mathrm{nm}\\ \int \mathrm{Ee}\left(\lambda \right).Math.d\lambda \\ \lambda =250\mathrm{nm}\end{array}}{\begin{array}{c}\lambda =780\mathrm{nm}\\ k_m\int \mathrm{Ee}\left(\lambda \right).Math.V\left(\lambda \right).Math.d\lambda \\ \lambda =380\mathrm{nm}\end{array}}\mathrm{is}\le 2.Math.{10}^{-6}W/\mathrm{lm},$ wherein: Ee (λ) as measured in W/nm is a spectral distribution of a radiant flux, V (λ) is a dimensionless spectral luminous efficiency, k.sub.m provided as 683 lm/W is a photometric radiation equivalent, and λ as measured in nm is a wavelength, and wherein value k2 is calculated using intervals of the wavelength λ of five nanometers.

46. The automotive solid-state headlamp of claim 45, wherein the factor k2 is ≤2.Math.10.sup.−7 W/lm.

47. The automotive solid-state headlamp of claim 33, wherein the light-transmissive housing comprises a UV-attenuating material having a UV transmission of not more than 90% per 1 mm at a wavelength of 380 nm, of not more than 50% per 1 mm at a wavelength of 315 nm, and of not more than 5% per 1 mm at a wavelength of 250 nm.

48. The automotive solid-state headlamp of claim 33, wherein the light-transmissive housing comprises a UV-attenuating glass or a UV-attenuating hard glass.

49. The automotive solid-state headlamp of claim 33, wherein the solid state light sources are configured to emit white light with a spectral energy distribution that has a correlated colour temperature of at least 5000 degrees Kelvin.

50. The automotive solid-state headlamp of claim 49, wherein the correlated colour temperature is not in excess of 6000 degrees Kelvin.

51. The automotive solid-state headlamp of claim 33, further comprising: a reflector optics arranged at the front portion, wherein the solid state light sources are configured to emit light towards the reflector optics, wherein the reflector optics comprises a first reflector optic portion and a second reflector optic portion, the first reflector optic portion being configured to receive the light emitted from the light sources and to emit the light toward the second reflector optic portion, and wherein the second reflector optic portion is configured to receive the light reflected off the first reflector optic portion and to emit the light through the light-transmissive housing.

52. The automotive solid-state headlamp of claim 51, wherein the first reflector optic portion comprises a plurality of first reflective surfaces which each include an inclination angle with respect to the longitudinal direction, and wherein an inclination of the first reflective surfaces with respect to the longitudinal direction decreases with increasing distance from the longitudinal direction.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0026] Further advantages, features and details of the various aspects become apparent from the claims, from the following description of preferred embodiments and from the drawings. In the figures, the same reference signs denote the same features and functions.

[0027] There is shown in:

[0028] FIG. 1 a perspective view of an H7-type solid-state headlamp lamp according to an embodiment;

[0029] FIG. 2 a side view of the solid-state headlamp lamp of FIG. 1;

[0030] FIG. 3 a side view of the solid-state headlamp lamp of FIG. 1 rotated by 90 degrees about its longitudinal axis compared to the view in FIG. 2;

[0031] FIG. 4 a side view of the solid-state headlamp similar to FIG. 2, but showing lengths and diameters of individual sections of the lamp;

[0032] FIG. 5 a top view of the solid-state headlamp from FIG. 1;

[0033] FIG. 6 a top view from below of the solid-state headlamp of FIG. 1;

[0034] FIG. 7 a perspective view of a reflector optic of the solid-state headlamp of FIG. 1;

[0035] FIG. 8 a cross-sectional view of the reflector optics of FIG. 7 with the beam path of the light emitted by solid-state light sources indicated therein;

[0036] FIG. 9 a cross-sectional view of the reflector optics from FIG. 7 showing the lengths and diameters of individual sections of the reflector optics;

[0037] FIG. 10A a schematic cross-sectional view of the reflector optics of FIG. 7 showing the angles of inclination of first reflecting surfaces on the reflector body with respect to the longitudinal axis X;

[0038] FIG. 10B a very schematic, enlarged, but not drawn to scale, section of FIG. 10A illustrating the angle of inclination as indicated therein;

[0039] FIG. 11A a schematic cross-sectional view of the reflector optics of FIG. 7 showing the angles of inclination of second reflective surfaces on the pin with respect to the longitudinal axis X;

[0040] FIG. 11B a very schematic, enlarged, but not drawn to scale, section of FIG. 11A illustrating the angle of inclination indicated therein;

[0041] FIG. 12 perspective view of the combination of reflector optics and support member (printed circuit board) with solid-state light sources arranged thereon;

[0042] FIG. 13 a diagram showing the radiation characteristics of the solid-state headlamp from FIG. 1;

[0043] FIG. 14 in a perspective view the support element of FIG. 12 with solid-state light sources arranged thereon as well as the corresponding current supply lines;

[0044] FIG. 15 in oblique plan view the support member (printed circuit board) with a special arrangement of the solid-state light sources arranged thereon;

[0045] FIG. 16 in a perspective view, a light transmissive housing of the solid state headlamp of FIG. 1;

[0046] FIG. 17 a cross-sectional view (top) and a top view (bottom) of the light transmissive housing of FIG. 16 with dimensions;

[0047] FIG. 18 a perspective view of a heat sink section of the solid state headlamp of FIG. 1;

[0048] FIG. 19 a side view of the heat sink portion of FIG. 18;

[0049] FIG. 20 a side view of the heat sink portion of FIG. 18 rotated by 90 degrees about its longitudinal axis compared to the view shown in FIG. 19;

[0050] FIG. 21 a side view of the heat sink portion of FIG. 18 similar to FIG. 19, but showing lengths and diameters of individual sections of the portion;

[0051] FIG. 22 a top view of the heat sink portion of FIG. 18;

[0052] FIG. 23 a bottom view of the heat sink portion of FIG. 18;

[0053] FIG. 24 in a perspective view, a socket or mounting portion of the solid state headlamp of FIG. 1;

[0054] FIG. 25 a copy of FIG. 2 of ECE Regulation 37 from Addendum 36 (dated 3 Jul. 2012) for a lamp of the H7 type (prior art); and

[0055] FIG. 26 a copy of FIG. 2 of ECE Regulation 37 from Addendum 36 (dated 3 Jul. 2012) for a lamp of the H11 type (prior art).

DETAILED DESCRIPTION OF ILLUSTRATIVE EMBODIMENTS

[0056] In the following description of preferred embodiments, it should be understood that the present disclosure of the various aspects is not limited to the details of the structure and arrangement of the components as shown in the following description and drawings. The embodiments may be put into practice or carried out in various ways. It should further be appreciated that the expressions and terminology used herein are used for the purpose of specific description only, and these should not be construed as such in a limiting manner by those skilled in the art.

[0057] The solid-state lamp 10 disclosed herein, as well as the corresponding reflector optical system 300, are for use in a power-driven vehicle having an internal combustion engine, a purely electric, fuel cell-, or hybrid drive, etc., and in particular for installation in a reflector cavity for vehicle front illumination such as a vehicle main headlamp or a fog lamp (hereinafter collectively referred to as vehicle headlamp) used for illuminating a road surface. The type of power-driven vehicle may be, without limitation of generality, a passenger car such as a sedan, a station wagon, a sports utility vehicle (SUV), a minivan, a pickup truck, an all-terrain vehicle, a bus or a truck, or a leisure vehicle such as a snowmobile or a motorcycle, and the like. Alternatively, the term “power-driven vehicle” in this disclosure also includes watercraft, such as motorboats, jet skis, or aircraft, such as airplanes or helicopters.

I. Structure of the Solid-State Lamp

[0058] FIGS. 1 to 6 show an overview of a solid-state headlamp 10 according to aspects of the present disclosure. The solid-state headlamp 10 shown herein is of the H7 type (as actually specified for halogen headlights), and the basic structure shown in the figures is generally transferable to other types in accordance with further embodiments, for example to solid-state headlamps of the H8, H9, H11 or H16 type. Accordingly, in FIGS. 1 to 3 and 5 to 6, the socket 20 (PX26d for type H7) is drawn only in dashed lines to emphasize the interchangeability of the socket for the implementation of other types (e.g. PGJ19-1 for type H8; PGJ19-5 for H9; PGJ19-2 for H11 or PGJ19-3 for H16) with an otherwise similar or identical lamp design.

[0059] The solid-state headlamp 10 of type H7 described here is suitable, for example, for use in generating high beam or low beam. In the case of type H8, the corresponding solid-state headlamp 10 is suitable for use, for example, for fog lights. In the case of type H9, the corresponding solid-state headlamp 10 is suitable for use, for example, for generating high beam. In the case of type H11, the corresponding solid-state headlamp 10 is suitable for generating, for example, fog light, high beam light or low beam light. Finally, in the case of type H16, the corresponding solid-state headlamp 10 is suitable, for example, for generating fog light. However, alternative applications are equally conceivable.

[0060] With reference to FIG. 1, the solid-state headlamp 10 is composed of a reflector optical system 300 (also referred to herein as reflector optics) having a reflector body 30 and a pin 360, a light-transmissive housing 40, a support member 50 formed as a circuit board having solid-state light sources 70 disposed thereon, a heat sink portion 60, and the base or mounting element 20. These components together form a lamp body 1 extending in a longitudinal direction or along a longitudinal axis X. This longitudinal axis X may correspond to the reference axis defined in the ECE regulation 37 mentioned at the outset and described below.

[0061] As can be seen in FIGS. 1 through 6, the solid-state headlamp 10 is formed of a generally rotationally symmetrical shape about the longitudinal axis X. The reflector optics including the reflector body 30 and the pin 360, and the light transmissive housing 40 form a front portion of the lamp body 1. The heat sink portion 60 and the socket 20 form a rear base portion of the lamp body 1. The support member 50 with the solid-state light sources 70 arranged thereon is arranged at a front end of the heat sink portion 60. The main surfaces of the support member 50 are perpendicular to the longitudinal axis X. Therefore, the solid-state light sources 70 arranged on the support member 50 emit their light into a space directed along the longitudinal axis X.

[0062] The distal end of the solid-state headlamp 10 is formed by the cap-shaped reflector optical system 300, which close off the light transmissive housing 40 in the distal direction. As will be explained in more detail below, the reflector optical system 300 serve to reflect the light emitted by the solid-state light sources 70 so that it emerges substantially in a plane perpendicular to the longitudinal axis X with maximum luminous intensity, but provides a sufficiently wide beam angle when viewed in any plane enclosing the longitudinal axis X. The radiation in all directions perpendicular to the longitudinal axis X is thereby quite homogeneous.

[0063] The light-transmissive housing 40 is also provided at the front end of the heat sink portion 60, so that the support member 50 with the solid-state light sources 70 arranged thereon is disposed within the light-transmissive housing 40. In addition to the solid-state light sources 70, a drive circuitry 55 electronically coupled to the light sources 70 and arranged with the support member 50 at the rear base portion of the lamp body 1, namely the front end of that portion, is also provided on the support member 50. The drive circuitry is adapted to drive the plurality of light sources 70 when supplied with power. The drive circuitry 55 is only indicated in FIG. 15 via the wiring of individual LED chips 72, but the basic structure of a drive circuitry 55 for arrays of solid-state light sources is generally known, so that reference can be made here to the relevant literature. If the support member 50 with the drive circuitry 55 and the solid-state light sources 70 arranged thereon is assigned to the front portion, then such front portion is essentially associated with a function of generating light from supplied power as well as optical reflection for emitting the light from the lamp.

[0064] The rear base portion, on the other hand, essentially has a function of dissipating the heat generated by the drive circuitry 55 and the solid-state light sources 70, as well as mechanically and electrically coupling the lamp 10 to the vehicle side via the socket 20. The components are described individually below.

II. Reflector Optics

[0065] With reference to FIGS. 7 through 12, the structure and function of a reflector optical system 300 including reflector optics 39 that can be used in the solid-state headlamp 10 shown in FIGS. 1 through 6 is described. The system 300 includes the reflector body 30, which is rotationally symmetric about the longitudinal axis X and has a spherical outer surface 31 facing the distal direction. In the particular embodiment, it has a semi-spherical shape. On the side facing the proximal direction, i.e., facing the support member 50 and the solid-state light sources 70 in the assembled state, the reflector body 30 has a first reflector optic portion 32 having a substantially concave shape 320. The concave shape 320 is shaped in the manner of a concave mirror, but has an overall conical shape rather than a spherical segment shape or a paraboloid because, as can be seen in FIG. 8, no focal plane or singular focal point is intended.

[0066] Rather, the concave shape 320 of the first reflector optic portion 32 is composed of a plurality of first reflective surfaces 35a-35e, which are annularly arranged around the longitudinal axis X and concentric to each other. In the particular embodiment example, there are 5 first reflective surfaces 35a-35e, each of which is adjacent to the other. Furthermore, the first reflective surfaces 35a-35e each have a conical shape with a half cone angle or an inclination angle ϑ relative to the longitudinal axis X, which decreases with increasing distance from the longitudinal axis X. FIG. 10A shows, in one embodiment, how the inclination angle ϑ decreases from the innermost first reflective surface 35e at the smallest distance from the central or longitudinal axis X with ϑ.sub.5=69.5 deg. over the next adjacent first reflective surface 35d at a slightly larger distance from the central or longitudinal axis X with ϑ.sub.4=67.4 degrees, further over the next adjacent first reflecting surface 35c with again a slightly larger distance to the center or longitudinal axis X with ϑ.sub.3=65.8 degrees, further over the next first reflecting surface 35b with again a slightly larger distance to the center or longitudinal axis X with ϑ.sub.2=64.6 degrees, up until the outermost first reflecting surface 35a with the largest distance to the center or longitudinal axis X with an inclination angle of ϑ.sub.1=63.7 degrees. FIG. 10B schematically shows in an enlarged view how the angle ϑ is determined. Note that FIG. 10A graphically shows the full cone angle, i.e., 2×ϑ.

[0067] The outer edge of the outermost first reflective surface 35a is bounded by a proximal end surface 33a. The inner edge of the innermost first reflective surface 35d is bounded by a conically shaped root portion 36a of a pin 360 to be explained below. The first reflective surfaces 35a-35e are provided with a highly reflective mirrored coating facing the light sources with a corresponding inclination. The reflectance amounts to 90% or more, preferably 95% or more. For example, in vacuum processes, the surface to be reflected can be coated with 99.98% pure aluminum or silver. The mirrored surface is sealed with a protective layer, for example silicone-based monomers (usually HMDS, VSI II or a combination).

[0068] In this way, the full irradiated surface of the concave shape 320 can be effectively used as the first reflective optic portion 32. It should be noted that the first reflective surfaces 35a-35e do not necessarily have to include a conical shape, they may also include a general skirt-shape, which also allows a concave or convex curved surface. According to further embodiments, a continuous skip-free surface may also be provided in the concave shape 320, in which the first reflective surfaces 35a-35e may smoothly merge into each other, accordingly.

[0069] Between the distal dome-shaped outer surface portion 31 of the reflector body 30 and the proximal end surface 33a there extends a substantially cylindrical flange portion 33 recessed from the dome-shaped outer surface portion 31 by a stepped portion 34. The flange portion 33 permits attachment of the light transmissive housing 40, into whose inner opening 43 at the distal end 41 the flange portion 33 can be fitted.

[0070] As can be seen in FIG. 8, which shows a beam of parallel light rays incident on the reflector optics along the longitudinal axis X and originating from the plurality of solid-state light sources 70, the annular first reflecting surfaces 35a-35e reflect the incident light by their inclination in the direction towards the longitudinal axis X, wherein—as mentioned above—the reflected beams do not meet in a common focal point on the longitudinal axis X, but arrive in mutually adjacent regions along the longitudinal axis X, so that the radiation density along the longitudinal axis X is distributed substantially homogeneously.

[0071] As can be seen from FIGS. 7 to 11, starting from the reflector body 30 in the center of the concave shape 320 or in the center of the annular first reflective surfaces 35a-35e, a pin 360 extends along the longitudinal axis X. The pin 360 is formed in a rotationally symmetrical shape. The pin 360 is rotationally symmetric and comprises substantially 3 sections. A first section is the aforementioned conical root portion 36a, which attaches directly to the center of the concave shape 320 on the reflector body 30. This conical root portion 36a tapers to an intersection of the pin 360 with a (virtual) plane perpendicular to the longitudinal axis X, defined by the proximal end face 33a at the edge of the concave shape 320. Beyond this intersection—as seen from the reflector body 30—a second reflector optic portion 36 extends along the longitudinal axis X, formed in principle by two immediately adjacent light emission regions 36b, 36c which contribute differently to the reflection. The first reflector optic portion 32 faces the second reflector optic portion 36 in at least a first (36b) of the two light emission regions. The pin 360, or more precisely the second reflector optic portion 36, represents the filament wire of conventional halogen headlight lamps that comply with the ECE standard Addendum 36: Regulation No. 37 (rev. 7) of Jul. 3, 2012, according to its function, position, length, and diameter, if applicable.

[0072] In this particular embodiment, the reflector body 30 and the pin 360 are monolithic, i.e. formed in one piece, e.g., made of an optical glass or a heat and/or UV resistant injection molded plastic material. The reflector body 30 may be opaque to prevent light leakage in the distal direction. It should be noted that the reflector body 30 and the pin 360 may as well be made of different materials not pertinent in the art. The tapered root portion 36a essentially has the function of holding the second reflector optic portion 36 centered on the longitudinal axis X while contributing as little as possible to shading. Other embodiments provide alternative supports for the second reflector optic portion 36, such as thin wires or a support extending from a side of the support member 50, but these may possibly always result in unwanted shading. Either way, however, the reflector optic portion 36 may be placed with great advantage on the longitudinal axis X extending from the reflector body 30 beyond the plane defined by its proximal end surface 33a (intersection point with longitudinal axis X), where the light reflected from the first reflective surfaces 35a-35e is incident in a relatively homogeneously distributed manner over this area.

[0073] The second reflector optic section 36 has a plurality of second reflective surfaces 37a-37e in spatial light receiving relationship with the plurality of first reflective surfaces 35a-35e. This means that the first reflective surfaces face the second reflective surfaces 37a-37e and vice versa, the function here being that, as can be seen in FIG. 8, the light supplied along the longitudinal axis X of the reflector optics 39 is reflected twice and, at the end, reflected or emitted substantially perpendicularly to the longitudinal axis X by the second reflective surfaces 37a-37e, in the case of the light transmissive housing 40 being attached, through the latter.

[0074] The second reflector optic section 36, including the second reflective surfaces 37a-37e, is set up rotationally symmetrical about the longitudinal axis X. The second reflective surfaces 37a-37e are formed annularly about the longitudinal axis X and have a conical shape or the skirt-like shape mentioned above. Each of the second reflective surfaces 37a-37e has the shape of a truncated cone, and the second reflective surfaces 37a-37e are arranged along the second reflector optic section 36 in a sequential manner on the pin 360.

[0075] The second reflective surfaces 37a-37e each taper toward the first reflector optic portion 32 and are aligned along the longitudinal axis X. To compensate for the increase in diameter along the longitudinal axis X caused by the taper of each of the second reflective surfaces 37a-37e, a step or undercut 39b-39e is provided between each of two adjacent second reflective surfaces 37a-37e, which in itself does not contribute to the reflection of radiation originating from the first reflector optic portion 32, but according to an alternative embodiment can be used for direct reflection of light incident from the light sources 70 not directly parallel to the longitudinal axis X but rather obliquely. At least, the scattered light from these undercuts can be used for radiation of the lamp outside the horizontal plane, i.e. for beam expansion.

[0076] As shown in FIG. 11A, the second reflective surfaces 37a-37e also each include an inclination angle ϑ with the longitudinal axis X. In this regard, in a particular embodiment, FIG. 11A shows how the inclination angle ϑ decreases from the second reflective surface 37e closest to the first reflector optic portion with ϑ.sub.10=24.5 degrees, through the next second reflective surface 37d with ϑ.sub.9=22.4 degrees, further through the next first reflective surface 37c with ϑ.sub.8=20.8 degrees, further through the next first reflective surface 37b with ϑ.sub.7=19.6 degrees, to the outermost first reflective surface 37a with ϑ.sub.6=18.7 degrees. FIG. 11B shows schematically in an enlarged view how the angle ϑ is determined. Note that FIG. 11A also graphically shows the full cone angle, i.e., 2×ϑ.

[0077] Similar to the first reflective surfaces 35a-35e, the inclination angle of the second reflective surfaces 37a-37e decreases with increasing distance from the first reflector optic portion 32 along the longitudinal axis X. As can be seen in FIG. 8, a direct spatial light-receiving relationship also exists between individual pairs of first and second reflective surfaces. The corresponding numbers of first reflective surfaces 35a-35e and second reflective surfaces 37a-37e are the same.

[0078] Thus for example, the innermost first reflective surface 35e is associated with the most distally positioned second surface 37e. The difference in inclination angles ϑ.sub.5 and ϑ.sub.10 amounts to 45 degrees—the same as required for double reflection with subsequent horizontal radiation from the light transmissive housing 40. Similarly, the next-innermost first reflective surface 35d is associated with the next-distal second reflective surface 37d (see FIG. 8). Again, the difference in inclination angles ϑ4 and ϑ.sub.9 is exactly 45 degrees. Consequently, this setup enables optimum radiation of the light from the solid-state headlamp 1 in the horizontal direction (see 90 degrees or −90 degrees in FIG. 13).

[0079] Conceivably, according to an alternative embodiment example, the inclination angles ϑ.sub.1 to ϑ.sub.6 or ϑ.sub.6 to ϑ.sub.10 could also simply be kept constant among each other, so that the difference of 45 degrees is maintained here as well.

[0080] However, at least in the case of the first reflective surfaces, the variation in the angle of inclination has the advantage that the spatial distance between the outermost first reflective surface 35a and the most proximal second reflective surface 37a does not become too large, so that sufficiently intense reflection is also ensured towards the front end of the pin 360, which therefore emits light as homogeneously as possible along the length of the second reflector optic section 36.

[0081] The pin 360 also has a free end 38a (a tip) that faces the support element 50 or the solid-state light sources 70 when the reflective optical system 300 is installed in the lamp. Adjacent to the free end 38a, a third reflective surface 38 is provided. It has the shape of a cone whose orientation is inverted compared to that of the plurality of second reflective surfaces 37a-37e, i.e., it tapers towards the tip or free end 38a. Here, the angle of inclination with respect to the longitudinal axis X is 45 degrees. In FIG. 12, it can be seen that the third reflective surface 38 is directly opposite a central region CLS of the support element 50, in which—as can be seen in FIG. 15—a subset of four LED chips 72a-72d is arranged. The third reflective surface 38 reflects the emitted light thereof directly and immediately in the horizontal direction through the light transmissive housing 40 in a 360-degree circle without shading, but also with sufficient radiation angles in the plane including the longitudinal axis X.

[0082] In FIG. 9, dimensions of the reflector optical system 300 are illustrated. The diameter s3 of the system 300 or the reflector body is, for example, 13 mm or 13.5 mm, and its length q including the pin 360 amounts to 11.5 mm. The diameter s3 should preferably be no more than 15 mm, thus complying with ECE regulation 37 for H7 and H11 types. The length p of the second reflector optical section 36 amounts to 4.5 mm in the embodiment and should preferably be between about 4.0 mm and about 5.9 mm, and the total length of the pin including the root portion 36a amounts to 6.5 mm in the example here. The maximum diameter s4 of the pin 360 or the second reflector optic portion 36 is 1.5 mm in the embodiment, but it should in any case preferably have a nominal diameter s4 of not more than 5 mm, further preferably of not more than 2.5 mm.

III. Photometric Properties of the Solid-State Headlamp

[0083] The solid-state headlamp 10 may be suitable as a retrofit lamp for the headlight applications described above. In other words, it can replace H7, H8, H9, H11 or H16 type halogen lamps in vehicle front headllights, with the corresponding types of sockets 20 to be set up in FIGS. 1 to 6.

[0084] In particular, the drive circuitry 55 and the solid-state light sources 70, together with the reflector optics 39, are designed so that, when powered, they cause the solid-state headlamp 10 to emit through the light-transmissive housing 40:

[0085] (a) a luminous flux of at least 1500 lumens +/−10% when supplied with a test voltage of 13.2 volts, or of at least 1750 lumens +/−10% when supplied with a test voltage of 28 volts, the lamp 10 not spatially extending in its external dimensions beyond an envelope as shown in FIG. 2 on page 35 of Annex 36: ECE Regulation 37 (dated 3 Jul. 2012) for a lamp of the H7 type; or

[0086] (b) a luminous flux of at least 800 lumens +/−15% when supplied with a test voltage of 13.2 volts, the lamp 10 not spatially extending in its external dimensions beyond an envelope as shown in FIG. 2 on page 39 of Annex 36: ECE Regulation 37 (of 3 Jul. 2012) for an H8 type lamp; or

[0087] (c) a luminous flux of at least 2100 lumens +/−10% when supplied with a test voltage of 13.2 volts, the lamp 10 not spatially extending in its external dimensions beyond an envelope as shown in FIG. 2 on page 43 of Annex 36: ECE Regulation 37 (of 3 Jul. 2012) for a lamp of the H9 type; or

[0088] (d) a luminous flux of at least 1350 lumens +/−10% when supplied with a test voltage of 13.2 volts or at least 1600 lumens +/−10% when supplied with a test voltage of 28 volts, the lamp 10 not spatially extending in its external dimensions beyond an envelope as shown in FIG. 2 on page 50 of Annex 36: ECE Regulation 37 (dated 3 Jul. 2012) for a lamp of the H11 type; or

[0089] (e) a luminous flux of at least 500 lumens +10%/−15% when supplied with a test voltage of 13.2 volts, the lamp 10 not spatially extending in its external dimensions beyond an envelope as shown in FIG. 2 on page 70 of Annex 36: ECE Regulation 37 (dated 3 Jul. 2012) for a lamp of the H16 type.

[0090] The special requirements are that in the narrow space of the lamp 10 defined by the envelope, a comparatively high power consumption takes place and the light is emitted by suitable reflector optics 39 with as little loss as possible, i.e., without absorption within the lamp, while the generated heat is efficiently dissipated without any impairment of the electrical components or the material.

[0091] A particular effect is achieved in that the second and third reflective surfaces 37a-37e, 38 on the pin 360 and in particular the light emitting regions 36b, 36c are defined according to their position with respect to a reference plane defined by the corresponding socket 20 (this applies to all types (a) to (e) as indicated above) and the longitudinal or reference axis is defined in a predetermined virtual box shown in Annex 36: ECE Regulation 37 (dated 3 Jul. 2012) on page 38 for the H7 type, on page 42 for the H8 type, on page 46 for the H9 type, on page 53 for the H11 type and on page 73 for the H16 type and supplemented with tolerance values in tables. The dimensions shown with reference to FIG. 9 (see description in section above) meet such box tolerances very well. It is important that the lamps according to the embodiments (for the indicated lamp types H7, H8, H9, H11, H16) comply with the distance of the tip of the second reflector optic portion 36 from the respective defined reference plane (RP) of 25 mm. The tolerance values bi of 0.25 mm are also complied with (or 0.2 mm for H7 and H11 at 12 volts nominal voltage). In the case of the H7 lamp, for example, the reference plane RP is defined by the distally oriented end face of the radial mounting lugs 23a, 23b and 24. The specifications regarding the reference plane for the respective lamp type (H7, H8, H9, H11 or H16) can be found in the respective FIG. 1 in Annex 36: ECE Regulation No. 37 (rev. 7) of Jul. 3, 2012 (correspondingly on pages 35, 39, 43, 50, and 70, respectively).

[0092] The length of the second reflector optic portion 36 can also be set in each case within the tolerance limits (values c1 (maximum length) and c2 (minimum length) in the tables: H7 12V: c1=4.6 mm, c2=4.0 mm; H7 24V: c1=5.9 mm, c2=4.4 mm; H8: c1=4.6 mm, c2=3.5 mm; H9: c1=5.7 mm, c2=4.6 mm; H11 12V: C1=5.0 mm, c2=4.0 mm; H11 24 V: c1=6.3 mm, c2=4.6 mm; H16: c1=3.6 mm, c2=2.6 mm). For the H7 12V type shown here purely as an example, the corresponding length p in FIG. 9 is 4.5 mm.

[0093] As a result, according to embodiments, the structure of the reflector optics in particular and the lamp body in general achieve a lamp structure that complies with ECE standards.

[0094] FIG. 13 shows the radiation pattern of a solid-state headlamp 10 of an embodiment. The plane of the drawing includes the longitudinal axis X and any axis Y perpendicular thereto, which lies in or parallel to the reference plane RP. The lamp 10 is schematically drawn in the center. The drawing plane of FIG. 13 is the same as that of FIG. 4. At 180 degrees, the distal direction is positioned (in FIG. 4, the upward direction), i.e., in principle, the front direction of the vehicle when the lamp is installed in its headlight reflector 200.

[0095] The rings around the center point indicate the luminous intensity in the respective direction. The narrow polygonal trace with solid lines shows the result of a simulation for the solid-state headlamp 10 embodied according to the embodiment in FIGS. 1 to 6, using the reflector optics 39 of FIGS. 7 to 12 and a support member 50 with an array of solid-state light sources 70 as shown in FIGS. 14 and 15. As can be seen in FIG. 13, the radiation angle in the substantially horizontal direction (90 degrees) is approximately 10 degrees. Here, the radiation angle (γ) is calculated based on the light emitted at a luminous intensity that is at least half of the maximum luminous intensity in the plane. This is illustrated by the example of the radiation pattern drawn by dashed lines: the point M denotes the maximum luminous intensity, the points H that angle at which the luminous intensity is only half of the maximum value. The radiation angle (γ) is schematically drawn, it amounts to 65 to 70 degrees.

[0096] By adapting the first and second reflective surfaces, adapting the optical lenses 71 in the solid-state light sources 70, or the coating or materials used, combined also with a further use of scattered light, an extension of the radiation angle (γ) to at least 40 degrees, at least 50 degrees or even at least 60 degrees is readily achievable for the skilled person, which is indicated in FIG. 13 by the dashed radiation characteristic. This may in particular be achieved, different from the embodiment shown in FIG. 10A, by again decreasing the inclination angle ϑ.sub.1 to ϑ.sub.5 of the first reflective surfaces (35a-35e) with increasing distance from the longitudinal axis X (in order to reflect the light further forward onto the pin 360 through the concave mirror arrangement), but then assigning inclination angles ϑ.sub.6 to ϑ.sub.10 to the second reflective surfaces, which also increase with increasing distance from the first reflector optic portion 32. With reference to FIG. 13, then, for example, light from second reflective surfaces (e.g., 37a, 37b) having comparatively larger inclination angles near the tip of the pin will also be reflected into angular ranges up to about 120 or 130 degrees (see FIG. 13). Conversely, second reflective surfaces (e.g., 37d, 37e) with comparatively smaller inclination angle near the first reflector optic portion 32 or near the root portion 36a of the pin 36 may then reflect light to an angular range up to 50 or 60 degrees (see FIG. 13).

[0097] This would also be possible the other way around, but the outer edges of the cap-shaped reflector optics 39 or the support member 50 would then shade large angles above/below the horizontal plane (90 degrees in FIG. 13). In any case, this approach may also be suitable for successful beam widening up to 60 or even 70 degrees (angle (γ)).

[0098] In other words, while the inclination angles of the first reflective surfaces (35a-35e) according to embodiments preferably decrease with increasing distance from the longitudinal axis X in order to obtain an optimal (maximum) radiation in the horizontal direction (and thus the lowest possible light losses in lamp), the course of the inclination angles of the second reflective surfaces (37a-37e) can be selected as a function of the distance from the first reflector optic portion 32 depending on a desired beam expansion, and accordingly increase, be constant, or decrease.

[0099] It should also be noted that, with advantage, the radiation characteristic of the light emitted by the light transmissive housing 40, is approximately rotationally symmetrical about the longitudinal axis (X), i.e., substantially free of shading effects.

[0100] The support member 50 shown in FIGS. 14 and 15 may preferably be a printed circuit board with high thermal conductivity, preferably with a base material having a thermal conductivity of not less than 7 W/(m.Math.K). It has, for example, a thickness of 1 mm. A rectangular array of LED chips 72 is placed on the support member 50, wherein in the specific embodiment 16 blue LED chips 72 (wavelength: 455 nm) are serially connected in 4 parallel strings (of 4 LED chips each). A phosphor-ceramic converter is bonded to the LED chips 72, which converts the blue light into ECE-compliant white light with a correlated color temperature (CCT) of 5000 to 6000 K. The light is then emitted by the LED chips 72. It should be noted here that the type of PCB, as well as the number and interconnection of the LED chips 72 may be arbitrary, as long as the luminous flux provided by them is maintained. Consequently, more or fewer LEDs may be provided, or LEDs with other correlated color temperatures, as well as mixtures of LEDs of different types, which, for example, may be combined to produce a white field.

[0101] However, it has been found to be particularly advantageous if silicone collimator lenses 71 are individually injection molded onto each of the LED chips 72 to reduce the beam angle of the LED chips 72 from typically 60 degrees to 10-20 degrees, i.e., to bring about some focusing of the light emitted from the solid-state light sources 70 toward the reflector optics 39 so that the light impinges substantially parallel to the longitudinal axis X onto the first reflector optics section 32.

[0102] By such a structure, a luminous efficiency of the light emitted through the light-transmissive housing 40 calculated on the consumption per electrical power supplied to the drive circuitry 55 may be at least 100 lumens per watt, preferably 120 lumens per watt, more preferably 150 lumens per watt, in the case of the solid-state headlamp 10.

[0103] The light transmissive housing 40 is shown in FIGS. 16 and 17. In the particular embodiment, it is a cylindrical envelope made of hard glass, which essentially serves as a dirt and dust shield for the inner chip and mirror space. In the particular embodiment, it has a length u of 9.5 mm and a wall thickness v of 0.6 mm, and a diameter s5 of 13 mm. The glass is preferably a UV-attenuating glass, or a UV-attenuating hard glass, in particular an aluminum silicate glass. A non-limiting example of an easy-to-use hard glass is Schott 8253.

[0104] In particular, the light-transmissive housing 40 may preferably comprise a UV-attenuating material having a UV transmittance of no more than 90% per 1 mm at a wavelength of 380 nm, of no more than 50% per 1 mm at a wavelength of 315 nm, and of no more than 5% per 1 mm at a wavelength of 250 nm. Schott 8253 satisfies such conditions. The second reflector optic portion 32 is in register with the light transmissive housing 40. It is positioned within the light transmissive housing 40 and the second reflective surfaces 37a-37e each face the light transmissive housing 40, albeit at an angle.

[0105] By using the blue LEDs with converter and the UV-attenuating hard glass, compliance with the following conditions specified in ECE Regulation 37 can be ensured according to embodiments:

[0106] For a factor k1 substantially expressing a relative amount of UV-A radiation power with respect to a luminous flux of visible light emitted through the light-transmissive housing 40 defined as

[00001]$k1=\frac{\begin{array}{c}\lambda =400\mathrm{nm}\\ \int \mathrm{Ee}\left(\lambda \right).Math.d\lambda \\ \lambda =315\mathrm{nm}\end{array}}{\begin{array}{c}\lambda =780\mathrm{nm}\\ k_m.Math.\int \mathrm{Ee}\left(\lambda \right).Math.V\left(\lambda \right).Math.d\lambda \\ \lambda =380\mathrm{nm}\end{array}},$

[0107] a condition: k1≤2.Math.10.sup.−4 W/lm is satisfied,

[0108] wherein:

[0109] Ee (λ) as measured in W/nm is the spectral distribution of the radiant flux;

[0110] V (λ) is the dimensionless spectral luminous efficiency;

[0111] k.sub.m provided as 683 lm/W is the photometric radiation equivalent; and

[0112] λ as measured in nm is the wavelength,

[0113] wherein value k1 is calculated using intervals of the wavelength λ of five nanometers.

[0114] Preferably, the factor k1≤2.Math.10.sup.−5 W/lm.

[0115] For a factor k2 substantially expressing a relative amount of UV-B radiation power with respect to a luminous flux of visible light emitted through the light-transmissive housing 40 defined as

[00002]$k2=\frac{\begin{array}{c}\lambda =315\mathrm{nm}\\ \int \mathrm{Ee}\left(\lambda \right).Math.d\lambda \\ \lambda =250\mathrm{nm}\end{array}}{\begin{array}{c}\lambda =780\mathrm{nm}\\ k_m.Math.\int \mathrm{Ee}\left(\lambda \right).Math.V\left(\lambda \right).Math.d\lambda \\ \lambda =380\mathrm{nm}\end{array}},$

[0116] a condition: k2≤2.Math.10.sup.−6 W/lm is satisfied,

[0117] wherein:

[0118] Ee (λ) as measured in W/nm is the spectral distribution of the radiant flux;

[0119] V (λ) is the dimensionless spectral luminous efficiency;

[0120] k.sub.m provided as 683 lm/W is the photometric radiation equivalent; and

[0121] λ as measured in nm is the wavelength,

[0122] wherein value k2 is calculated using intervals of the wavelength λ of five nanometers.

[0123] Preferably, the factor k2≤2.Math.10.sup.−7 W/lm. This ensures that the plastic components of the headlight reflector etc. surrounding the lamp 10 are not detrimentally affected by the UV radiation.

IV. Heat Sink Portion

[0124] FIGS. 18 to 23 show the heat sink portion 60 in detail. It substantially concerns a cooling body made of a material with high thermal conductivity of preferably 200 W/(m.Math.K) or more, for example aluminum, or further preferably 300 W/(m.Math.K), for example copper with e.g. 340 W/(m.Math.K) or a copper alloy.

[0125] The heat sink portion 60 comprises a distal base portion 62 and a proximal base portion 63, which differ in diameter but otherwise both have substantially the same cylindrical structure, each characterized by a number of annular, circumferential and mutually parallel cooling ribs 62a-62d and 63a-63c, respectively. The diameter s1 of the proximal base portion 63 with the cooling ribs 63a-63c is 19.8 mm and the diameter s2 of the distal base section 62 with the cooling ribs 63a-63c is 14.5 mm.

[0126] A mounting portion 61 whose diameter s6 is 11.5 mm is located at the front end, so that it can be fitted into the opening 43 at the proximal end of the light transmissive housing 40. A distal end face 65 is configured to receive the support member 50 with its rear side. By maximizing the contact area, heat can be efficiently dissipated from the LED chips 72. Bores 67a, 67b are provided in the distal end face 65 to receive current supply leads 57a, 57b for the drive circuitry 55 and the solid-state light sources 70 shown in FIG. 14. These have contact portions 58a, 58b formed in corresponding contact mounting holes 54a, 54b in the support member 50 (FIG. 15). The current supply leads contact the printed circuit board at the plus and minus terminals. In the socket 20 (see FIG. 24), they are connected to the contact tabs 25a, 25b via the bottom contact welding 26a, 26b as shown in FIG. 4. The current leads 57a, 57b may also be formed of copper and have a tin-plated surface coating for improved solderability and weldability. In this particular embodiment, their diameter may be 0.6 to 0.7 mm and their length 35 mm. The dimensions can be adapted to the specific requirements. However, they contribute to heat conduction by conducting heat from the printed circuit board to the socket contacts 26a, 26b and the contact tabs 25a, 25b.

[0127] A mounting portion 64 is provided at the opposite end of the heat sink portion 60, which is configured to be received and secured in an accommodation space 27 of the socket 20 (see FIG. 24). In FIGS. 22 and 23, it can be seen that corresponding bores 67a, 67b are also provided in the proximal end face 66 through which the current supply leads 57a, 57b are passed.

[0128] In the distal base portion 62 of the heat sink section 60, the annular circumferential cooling ribs 62a-62b are formed on a hollow cylindrical portion 620 which, as indicated in FIG. 4, has a cylindrical bore 621 inside which extends along the longitudinal axis to near the distal end, i.e., the mounting portion 61 with the distal end face 65, to which the support member 50 is attached. The inner diameter of this bore may be 9 mm. The bore 621 permits particularly effective rear cooling of the distal end face 61 in combination with the slots formed by a heat transfer opening 631 between the cooling ribs 63a-63c. It is provided in the proximal base portion 63 and is bounded by lateral walls 631. The heat transfer opening 631 allows air flow through the interior of the heat sink portion 60 and cooling of the bore 621. This structure allows particularly effective heat transfer from the support member and solid-state light sources 70 toward the socket 20 for dissipation of heat to the external environment and adjacent components. In this embodiment, the length l of the heat sink portion 60 excluding the mounting portion 64 amounts to 20.5 mm, which is thus comparatively long.

[0129] The socket 20 is shown in perspective in FIG. 24. In addition to contact tabs 25a, 25b and an insulating socket part 21, it has, for the special H7 type lamp with PX26d socket type, an annular flange portion 22 with radial mounting lugs 23a, 23b and 24 arranged thereon, adapted to be coupled to a vehicle-mounted reflector socket of a reflector 200 receiving the lamp.

[0130] Example 1: An automotive solid-state headlamp includes a lamp body extending in a longitudinal direction, the lamp body having a rear base portion and a front portion and including a support member disposed in a light-transmissive housing, a plurality of solid-state light sources arranged on the support member at the rear base portion of the lamp body, a drive circuitry electrically coupled to the light sources and arranged at the rear base portion of the lamp body and configured to operate the plurality of light sources when energized, wherein the plurality of light sources, when energized, are configured to cause the solid-state lamp to emit, through the light-transmissive housing (a) a luminous flux of at least 1500 lumens +/−10% when energized with a 13.2 Volt test voltage, or of at least 1750 lumens +/−10% when energized with a 28 Volt test voltage, or (b) a luminous flux of at least 1350 lumens +/−10% when energized with a 13.2 Volt test voltage, or of at least 1600 lumens +/−10% when energized with a 28 Volt test voltage.

[0131] Example 2: The automotive solid-state headlamp of Example 1, further comprising a reflector optics arranged at the front portion, wherein the solid state light sources are configured to emit light towards the reflector optics, wherein the reflector optics comprises a first reflector optic portion and a second reflector optic portion, the first reflector optic portion being configured to receive the light emitted from the light sources and to emit the light toward the second reflector optic portion, and wherein the second reflector optic portion is configured to receive the light reflected off the first reflector optic portion and to emit the light through the light-transmissive housing.

[0132] Example 3: The automotive solid-state headlamp of Example 2, wherein the second reflector optic portion is substantially bounded by a cylindrical portion and defines a light-emission region in register with the light-transmissive housing, wherein the light-emission region is arranged along the longitudinal axis of the lamp body and has a length, and wherein the length is between about 4.0 mm and 5.3 mm.

[0133] Example 4: The automotive solid-state headlamp of Example 3, wherein the light-emission region has a nominal diameter not exceeding 5 mm.

[0134] Example 5: The automotive solid-state headlamp of claim Example 4, wherein the nominal diameter is not greater than 2.5 mm.

[0135] Example 6: The automotive solid-state headlamp of claim Example 3, wherein the light-emission region is formed by a plurality of conical or skirt-shaped reflective surfaces formed on the second reflector optic portion.

[0136] Example 7: The automotive solid-state headlamp of Example 2, wherein the first reflector optic portion comprises a reflector body, the reflector body occluding a transmission of light, the reflector body being disposed opposite the plurality of solid-state light sources and covering a distal end of the light-transmissive housing.

[0137] Example 8: The automotive solid-state headlamp of Example 7, wherein the reflector body is opaque.

[0138] Example 9: The automotive solid-state headlamp of Example 7, wherein the reflector body is configured to support the first reflector optic portion and the second reflector optic portion.

[0139] Example 10: The automotive solid-state headlamp of Example 2, wherein reflective surfaces disposed on the first and second reflector optic portions have a specular reflectivity of at least 90% of incident light.

[0140] Example 11: The automotive solid-state headlamp of Example 10, wherein the specular reflectivity is at least 95%.

[0141] Example 12: The automotive solid-state headlamp of Example 1, wherein the lamp is devoid of an active cooling element.

[0142] Example 13: The automotive solid-state headlamp of Example 1, wherein the lamp body comprises a passive heat sink portion.

[0143] Example 14: The automotive solid-state headlamp of Example 1, wherein the first reflector optic portion comprises a plurality of annular reflective surfaces inclined towards the longitudinal axis and wherein the second reflector optic portion comprises a plurality of annular reflective surfaces, inclined relative the longitudinal axis towards the first reflector optic portion.

[0144] Although a preferred embodiment of the present disclosure has been described, it is understood that various changes, adaptations and modifications may be made thereto without departing from the spirit of the disclosure and the scope of protection of the appended claims. Therefore, the scope of protection of the disclosure should not be determined by reference to the above description, but should instead be determined by reference to the appended claims along with their full scope of protection of equivalents. Further, it is understood that the appended claims do not necessarily encompass the broadest scope of protection of the disclosure that the applicant is entitled to claim, or the only way in which the disclosure can be claimed, or that all of the features listed are necessary.