Athermal Optical Assembly

Abstract

This disclosure describes optical assemblies that generate output with substantial stability over a wide variation in temperature. The optical assemblies can be integrated, for example, as part of array generators arranged to project an array or other pattern of dots onto an object or projection plane.

Claims

1. A hybrid optical assembly comprising: a first transmissive substrate; a first aspherical lens on a first side of the first transmissive substrate; a second hybrid diffractive/refractive lens on a second side of the first transmissive substrate; a second transmissive substrate separated from the first transmissive substrate; a third aspherical lens on a first side of the second transmissive substrate; and a fourth aspherical lens on a second side of the second transmissive substrate; wherein the third aspherical lenses lens faces the second hybrid diffractive/refractive lens, and wherein the output of the hybrid optical assembly exhibits substantial stability over a temperature range of 20 C.-100 C.

2. The hybrid optical assembly of claim 1 wherein the first and second transmissive substrates are separated from one another by a distance in a range of 4 mm-10 mm.

3. The hybrid optical assembly of claim 1 wherein the first and second transmissive substrates are composed of clear borosilicate glass and the first, second, third and fourth lenses are composed of epoxy.

4. An optical pattern generator comprising: an array of light emitting elements; and a hybrid optical assembly according to claim 1, wherein the array of light emitting elements is disposed such that light generated by the light emitting elements passes through the fourth lens, the third lens, the second lens and the first lens of the hybrid optical assembly, in that order, so as to project a pattern of optical dots corresponding to the arrangement of the light emitting elements.

5. The optical array generator of claim 4 wherein the light emitting elements are VCSELs.

6. A method of generating a pattern of optical dots, the method comprising: emitting light from a plurality of light emitting elements arranged in an array or other pattern; passing the emitted light through a hybrid optical assembly comprising three aspherical lenses and a hybrid diffractive/refractive lens; and projecting the light that passed through the hybrid optical assembly onto an object or plane, wherein the projected light forms a pattern of dots.

7. (Currently amended The method of claim 6 including passing the emitted light through the hybrid optical assembly.

8. The hybrid optical assembly according to claim 1, wherein the first aspheric lens has a focal-length-normalized curvature of 9.21, the second hybrid diffractive/refractive lens has a focal-length-normalized curvature of 2.85, the third aspheric lens has a focal-length-normalized curvature of 0.34, and the fourth aspheric lens has a focal-length-normalized curvature of 0.78.

9. The hybrid optical assembly according to claim 1, wherein the first aspheric lens, the second hybrid diffractive/refractive lens, the third aspheric lens, and the fourth aspheric lens have focal-length-normalized diameters of 0.49, 0.49, 0.35, and 0.29, respectively.

10. The hybrid optical assembly according to claim 1, wherein the first aspheric lens, the second hybrid diffractive/refractive lens, the third aspheric lens, and the fourth aspheric lens have focal-length-normalized thicknesses of 0.0044, 1.048, 0.067, and 0.067, respectively.

11. The hybrid optical assembly according to claim 8 having an aspect ratio of 0.356.

12. The hybrid optical assembly according to claim 8, the first, third and fourth aspherical lenses have the following coefficients, respectively: TABLE-US-00009 1.sup.st aspheric 3.sup.rd aspheric 4.sup.th aspheric Coefficient (r) lens lens lens Fourth-order 0.103 0.114 0.382 Sixth-order 0 2.4032 3.544 Eighth-order 0 41.19 62.281 Tenth-order 0 324.92 523.773 Twelfth-order 0 1203.11 1930.264 Fourteenth-order 0 1694.44 2348.243 and wherein the second hybrid diffractive/refractive lens has the following coefficients: TABLE-US-00010 2.sup.nd hybrid diffractive/refractive Coefficient () lens Aspheric Fourth-order 0.115 Aspheric Sixth-order 0.859 Aspheric Eighth-order 5.705 Aspheric Tenth-order 17.849 Aspheric Twelfth-order 28.092 Aspheric Fourteenth-order 17.554 Diffractive-phase Second-order 525.287 Diffractive-phase Fourth-order 71.546 Diffractive-phase Sixth-order 30.983

13. The hybrid optical assembly according to claim 8 having an aspect ratio of 0.224.

14. The hybrid optical assembly according to claim 8, wherein the first, third and fourth aspheric lenses have the following coefficients, respectively: TABLE-US-00011 1.sup.st aspheric 3.sup.rd aspheric 4.sup.th aspheric Coefficient (r) lens lens lens Fourth-order 0.026 0.028 0.095 Sixth-order 0 0.237 0.350 Eighth-order 0 1.611 2.436 Tenth-order 0 5.034 8.115 Twelfth-order 0 7.384 11.847 Fourteenth-order 0 4.119 5.709 and wherein the second hybrid diffractive/refractive lens has the following coefficients: TABLE-US-00012 2.sup.nd hybrid diffractive/refractive Coefficient () lens Aspheric Fourth-order 0.027 Aspheric Sixth-order 0.085 Aspheric Eighth-order 0.223 Aspheric Tenth-order 0.277 Aspheric Twelfth-order 0.172 Aspheric Fourteenth-order 0.043 Diffractive-phase Second-order 834.621 Diffractive-phase Fourth-order 113.678 Diffractive-phase Sixth-order 49.228

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0012] FIG. 1 illustrates an example of an optical array generator that includes an athermal optical assembly.

[0013] FIG. 2 illustrates an example of an array of optical dots projected onto a projection plane by the optical array generator of FIG. 1.

[0014] FIG. 3 illustrates an example of an aspheric lens.

[0015] FIG. 4 illustrates properties of an example of a hybrid diffractive/refractive lens that can be included in the optical assembly.

[0016] FIGS. 5A, 5B and 5C are graphs illustrating performance of the optical assembly at different temperatures.

DETAILED DESCRIPTION

[0017] The present disclosure describes hybrid athermal optical assemblies that can be integrated, for example, into array generators arranged to project an array or other pattern of dots. Optical pattern projection can be used in a variety of applications such as three-dimensional (3D) or depth mapping, area illumination, and LCD backlighting. 3D (or depth) mapping, for example, refers to a set of 3D coordinates representing the surface of an object. As part of the process of depth mapping, light (i.e., visible, infra-red, or other radiation) can be projected onto a region with a pattern of high quality (e.g., good resolution, and with dots of optimal encircled energy) and well-controlled intensity, so that depth values can be found reliably over a substantial part of an object or objects in a scene and over a range of operating temperatures (e.g., from 20 C. to 100 C.).

[0018] As shown in FIG. 1, a hybrid optical assembly 20 includes several passive optical elements, i.e., lenses A, B, C and D. Two of the lenses, A and B, are disposed on opposite sides of a first transmissive (e.g., glass or wafer) substrate 32; the other two lenses, C and D, are disposed on opposite sides of a second transmissive (e.g., glass or wafer) substrate 34. The optical axes of the lenses A, B, C and D are aligned with one another, and the inner surfaces of the lenses B and C are separated from one another by a distance d, which for some applications is in the range of several (e.g., four) millimeters (mm) to about ten mm. In some implementations, although the optical axes may be aligned, the geometric path may not be aligned; for example, in implementations having a folded optical path, the geometric path is not aligned, whereas the optical axes of the lenses A, B, C and D are aligned. An array 22 of light emitting elements, such as a VCSELs, can be placed in front of the optical assembly 20 such that lens D is closest to the VCSEL array 22 and the lens A is furthest from the VCSEL array 22. Such an implementation can be particularly advantageous is some cases because the overall footprint of the assembly can be reduced (i.e., by increasing its thicknessthe dimension orthogonal to the footprint).

[0019] As illustrated in FIG. 2, the optical assembly 20 is arranged such that when light (e.g., IR light) from the VCSEL array 22 is emitted toward the optical assembly 20, an array of well-defined optical dots 38 appears on the projection plane 36. Collectively, the various lenses A, B, C and D help collimate and focus the light, such that the array of dots 38 appearing on the projection plane 26 corresponds, for example, to the arrangement of the VCSELs in the array 22. FIG. 2 illustrates a particular arrangement of the VCSEL array 22; other arrangements, and other numbers of VCSEL emitters within the array 22, can be provided for other implementations.

[0020] In the illustrated example, lenses A, C and D are implemented as aspherical lenses. In general, aspheric lenses can be designed, for example, with surfaces of the form:

[00001]$z\left(r\right)=\frac{r^2}{R\left(1+\sqrt{1-\left(1+\right).Math.\frac{r^2}{R^2}}\right)}+{}_1.Math.r^2-{}_2.Math.r^4+{}_{}.Math.r^6+\mathrm{.Math.}.Math.,$

where the optic axis is presumed to lie in the z-direction, and z(r) is the sag, i.e., the z-component of the displacement of the surface from the vertex, at distance r from the axis. The aspheric coefficients a, describe the deviation of the surface from the axially symmetric quadric surface specified by R and . See FIG. 3. On the other hand, lens B is implemented as a hybrid diffractive/refractive lens. Lens B can be described using the aspheric equation above in combination with the following polynomial expansion describing the diffractive phase of lens B:

[00002]$=M.Math.\underset{i=1}{\overset{N}{.Math.}}.Math..Math.A_i.Math.{}^{2.Math..Math.i}$

where M is the diffraction order of the hybrid diffractive/refractive lens, N is the number of polynomial coefficients in the series, A, is the coefficient on the 2i.sup.th power of , and is the normalized radial aperture coordinate. Specific examples of the lens characteristics and their respective properties for particular implementations are described below.

[0021] The specific properties of the lenses A through D are such that the optical assembly 20 is substantially athermal (i.e., its output exhibits substantial stability over a wide variation in temperature, for example, over the range 20 C. to 100 C.). Further, lenses (e.g., lenses A through D) also can provide for aberration correction.

[0022] Computer modeling was used to determine how different properties of the lenses and the optical assembly would vary with changes in temperature. Data describing implementations of hybrid optical assemblies are indicated in Tables I-VI, below. The dimensions (radius, thickness and diameter) associated with each surface based on the computer modeling is set forth in Table I and VI (in microns (m)). Further surface coefficients describing the shapes of lens surfaces and the characteristics of the hybrid refractive/diffractive element B are described in Tables II and V. Different dimensions may be appropriate for other implementations, however. Further the example hybrid optical assemblies described below can be modeled or simulated by, for example, sequential and/or non-sequential ray-tracing simulation software such as Zemax, the numerals included below describe the various components (e.g., thicknesses, diameters, surface shapes, coefficients) and their position within the illumination assembly, these numerals include a plurality of decimal places. For example the aspheric coefficients used to describe the aspheric surfaces of various components below can include as many as nine decimals places or more. However, although up to nine decimals places are included, in some cases far fewer decimal places are needed to adequately describe the various components and their respective position within the illumination assembly. For example, in some cases no more than two or three or four decimal places are required in order to effectively describe various components and their respective position within the hybrid optical assembly further described below.

[0023] Multiple surfaces define the optical assembly 20, including the lenses A through D. Table I, below, describes the various surfaces in the optical assembly 20 and the VCSEL array 22 for some implementations with a total track length of about 4 mm

TABLE-US-00001 TABLE I Surface Radius Thickness Diameter ID Type (mm) (mm) Glass (mm) Conic Comment OBJ STANDARD Infinity 377.6232 92.05419 0 1 STANDARD Infinity 0.1321681 D263TECO 1.385926 0 2 STANDARD Infinity 0.01258744 R14 1.365029 0 STO STANDARD Infinity 0.0314686 1.287502 0 4 EVENASPH 26.0797 0.01236523 R14 1.384618 0 lens A 6 STANDARD Infinity 0.00629372 R14 1.373109 0 base layer 7 STANDARD Infinity 0.1888116 D263TECO 1.374508 0 wafer AB 8 STANDARD Infinity 0.00629372 R14 1.416216 0 base layer 9 STANDARD Infinity 0.03689987 R14 1.417614 0 10 BINARY_2 8.06585 0 1.384618 0 lens B defined by 12 STANDARD Infinity 2.968914 1.425223 0 glass 13 EVENASPH 0.95528 0.1888116 R14 0.9911429 0 lens C 14 STANDARD Infinity 0.00629372 R14 0.9598653 0 base layer 15 STANDARD Infinity 0.1888116 D263TECO 0.9568284 0 wafer CD 16 STANDARD Infinity 0.00629372 R14 0.8663031 0 base layer 17 STANDARD Infinity 0.02517424 R14 0.8532662 0 18 EVENASPH 2.22158 0.1888116 0.8308089 0 lens D 19 STANDARD Infinity 0 0.7770572 0 IMA STANDARD Infinity N/A 0.7015326 0 VCSEL array

[0024] Thus, lens A is defined by surfaces 4 and 6; lens B is defined by surfaces 8, 9 and 10; lens C is defined by surfaces 13 and 14; and lens D is defined by surfaces 16, 17 and 18. Table II describes the various surface shapes, coefficients, and characteristics of the optical surfaces within the optical assembly 20 and the VCSEL array 22 for some implementations with a total track length of about 4 mm. In this implementation, the conic for each of the surfaces is zero. Further, although this implementation is described by an aspheric polynomial and a polynomial expansion describing the diffractive phase of lens B, other ways of describing the surfaces are within the scope of this disclosure.

TABLE-US-00002 TABLE II Surface ID Surface type OBJ STANDARD 1 STANDARD 2 STANDARD STO STANDARD 4 EVENASPH Coefficient on r{circumflex over ()}2 0 Coefficient on r{circumflex over ()}4 0.10313738 Coefficient on r{circumflex over ()}6 0 Coefficient on r{circumflex over ()}8 0 Coefficient on r{circumflex over ()}10 0 Coefficient on r{circumflex over ()}12 0 Coefficient on r{circumflex over ()}14 0 Coefficient on r{circumflex over ()}16 0 Aperture Floating Aperture Maximum Radius 0.6923092 6 STANDARD 7 STANDARD 8 STANDARD 9 STANDARD 10 BINARY_2 Diffraction Order 4 Coefficient on r{circumflex over ()}2 0 Coefficient on r{circumflex over ()}4 0.11494915 Coefficient on r{circumflex over ()}6 0.85854795 Coefficient on r{circumflex over ()}8 5.7044976 Coefficient on r{circumflex over ()}10 17.848874 Coefficient on r{circumflex over ()}12 28.092385 Coefficient on r{circumflex over ()}14 17.554371 Coefficient on r{circumflex over ()}16 0 Maximum term # 3 Normalization 0.69230919 Radius Coefficient on p{circumflex over ()}2 525.28684 Coefficient on p{circumflex over ()}4 71.54595 Coefficient on p{circumflex over ()}6 30.983 Aperture Floating Aperture Maximum Radius 0.6923092 12 STANDARD 13 EVENASPH Coefficient on r{circumflex over ()}2 0 Coefficient on r{circumflex over ()}4 0.11351174 Coefficient on r{circumflex over ()}6 2.4017377 Coefficient on r{circumflex over ()}8 41.190946 Coefficient on r{circumflex over ()}10 324.91913 Coefficient on r{circumflex over ()}12 1203.1116 Coefficient on r{circumflex over ()}14 1694.4363 Coefficient on r{circumflex over ()}16 0 14 STANDARD 15 STANDARD 16 STANDARD 17 STANDARD 18 EVENASPH Coefficient on r{circumflex over ()}2 0 Coefficient on r{circumflex over ()}4 0.38189163 Coefficient on r{circumflex over ()}6 3.5435835 Coefficient on r{circumflex over ()}8 62.280573 Coefficient on r{circumflex over ()}10 523.77256 Coefficient on r{circumflex over ()}12 1930.264 Coefficient on r{circumflex over ()}14 2348.243 Coefficient on r{circumflex over ()}16 0 19 STANDARD IMA STANDARD

[0025] Table III, below, describes further information pertaining to the foregoing implementation.

TABLE-US-00003 TABLE III Number of Surfaces 20 Stop 3 System Aperture Image Space F/# = 2.2 Effective Focal Length 2.832299 (in air at system temperature and pressure) Effective Focal Length 2.832299 (in image space) Back Focal Length 0.1514186 Total Track 3.999999 Image Space F/#: 2.2 Paraxial Working F/# 2.200017 Working F/# 2.20032 Image Space NA 0.2216194 Object Space NA 0.001704187 Stop Radius 0.6437044 Paraxial Image Height 0.3461546 Paraxial Magnification 0.007498492 Entrance Pupil Diameter 1.287409 Entrance Pupil Position 0.09568351 Exit Pupil Diameter 1214.659 Exit Pupil Position 2672.286 Field Type Real Image height in Millimeters Maximum Radial Field 0.3461546 Primary Wavelength 0.94 m Lens Units Millimeters Angular Magnification 0.00105794

[0026] The foregoing information (i.e., in Tables I, II and III) is non-limiting and is provided as examples to enable a person of ordinary skill to make and use the invention.

[0027] Table IV, below, describes the various surfaces in the optical assembly 20 and the VCSEL array 22 for some implementations with a total track length of about 6.356 mm.

TABLE-US-00004 TABLE IV Surface Radius Thickness Diameter ID Type (mm) (mm) Glass (mm) Conic Comment OBJ STANDARD Infinity 600 92.05419 0 1 STANDARD Infinity 0.21 D263TECO 1.385926 0 2 STANDARD Infinity 0.02 R14 1.365029 0 STO STANDARD Infinity 0.05 1.287502 0 4 EVENASPH 41.4377 0.01964693 R14 1.384618 0 lens A 6 STANDARD Infinity 0.01 R14 1.373109 0 base layer 7 STANDARD Infinity 0.3 D263TECO 1.374508 0 wafer AB 8 STANDARD Infinity 0.01 R14 1.416216 0 base layer 9 STANDARD Infinity 0.05862966 R14 1.417614 0 10 BINARY_2 12.8157 0 1.384618 0 lens B defined by 12 STANDARD Infinity 4.717264 1.425223 0 glass 13 EVENASPH 1.51784 0.3 R14 0.9911429 0 lens C 14 STANDARD Infinity 0.01 R14 0.9598653 0 base layer 15 STANDARD Infinity 0.3 D263TECO 0.9568284 0 wafer CD 16 STANDARD Infinity 0.01 R14 0.8663031 0 base layer 17 STANDARD Infinity 0.03999898 R14 0.8632662 0 18 EVENASPH 3.52984 0.3 0.8308089 0 lens D 19 STANDARD Infinity 0 0.7770572 0 IMA STANDARD Infinity N/A 0.7015326 0 VCSEL array

[0028] Thus, lens A is defined by surfaces 4 and 6; lens B is defined by surfaces 8, 9 and 10; lens C is defined by surfaces 13 and 14; and lens D is defined by surfaces 16, 17 and 18. Table V, below, describes the various surface shapes and characteristics of the optical surfaces within the optical assembly 20 and the VCSEL array 22 for some implementations with a total track length of about 6.356 mm. In this implementation, the conic for each of the surfaces is zero. Further, although this implementation is described by an aspheric polynomial and a polynomial expansion describing the diffractive phase of lens B, other ways of describing the surfaces are within the scope of this disclosure.

TABLE-US-00005 TABLE V Surface ID Surface type OBJ STANDARD 1 STANDARD 2 STANDARD STO STANDARD 4 EVENASPH Coefficient on r{circumflex over ()}2 0 Coefficient on r{circumflex over ()}4 0.025712148 Coefficient on r{circumflex over ()}6 0 Coefficient on r{circumflex over ()}8 0 Coefficient on r{circumflex over ()}10 0 Coefficient on r{circumflex over ()}12 0 Coefficient on r{circumflex over ()}14 0 Coefficient on r{circumflex over ()}16 0 Aperture Floating Maximum Radius 1.1 6 STANDARD 7 STANDARD 8 STANDARD 9 STANDARD 10 BINARY_2 Diffraction Order 4 Coefficient on r{circumflex over ()}2 0 Coefficient on r{circumflex over ()}4 0.02865682 Coefficient on r{circumflex over ()}6 0.084781608 Coefficient on r{circumflex over ()}8 0.22313584 Coefficient on r{circumflex over ()}10 0.27655249 Coefficient on r{circumflex over ()}12 0.17241308 Coefficient on r{circumflex over ()}14 0.042675803 Coefficient on r{circumflex over ()}16 0 Maximum term # 3 Normalization Radius 1.1 Coefficient on {circumflex over ()}2 834.62061 Coefficient on {circumflex over ()}4 113.67832 Coefficient on {circumflex over ()}6 49.228438 Aperture Floating Maximum Radius 1.1 12 STANDARD 13 EVENASPH Coefficient on r{circumflex over ()}2 0 Coefficient on r{circumflex over ()}4 0.028298476 Coefficient on r{circumflex over ()}6 0.23717158 Coefficient on r{circumflex over ()}8 1.6112157 Coefficient on r{circumflex over ()}10 5.0343342 Coefficient on r{circumflex over ()}12 7.3839288 Coefficient on r{circumflex over ()}14 4.1192835 Coefficient on r{circumflex over ()}16 0 14 STANDARD 15 STANDARD 16 STANDARD 17 STANDARD 18 EVENASPH Coefficient on r{circumflex over ()}2 0 Coefficient on r{circumflex over ()}4 0.095205578 Coefficient on r{circumflex over ()}6 0.34992886 Coefficient on r{circumflex over ()}8 2.4361528 Coefficient on r{circumflex over ()}10 8.115392 Coefficient on r{circumflex over ()}12 11.846725 Coefficient on r{circumflex over ()}14 5.7087296 Coefficient on r{circumflex over ()}16 0 19 STANDARD IMA STANDARD

[0029] Table VI, below, describes further information pertaining to the implementation described above.

TABLE-US-00006 TABLE VI Number of Surfaces 20 Stop 3 System Aperture Image Space F/# = 2.2 Effective Focal Length 4.500199 (in air at system temperature and pressure) Effective Focal Length 4.500199 (in image space) Back Focal Length 0.2405868 Total Track 6.355539 Image Space F/#: 2.2 Paraxial Working F/# 2.200017 Working F/# 2.20032 Image Space NA 0.2216194 Object Space NA 0.001704187 Stop Radius 1.022773 Paraxial Image Height 0.55 Paraxial Magnification 0.007498492 Entrance Pupil Diameter 2.045545 Entrance Pupil Position 0.1520301 Exit Pupil Diameter 1932.099 Exit Pupil Position 4250.677 Field Type Real Image height in Millimeters Maximum Radial Field 0.55 Primary Wavelength 0.94 m Lens Units Millimeters Angular Magnification 0.00105794

[0030] The foregoing information (i.e., in Tables IV, V and VI) is non-limiting and is provided as examples to enable a person of ordinary skill to make and use the invention

[0031] Among the listed lens materials, D263TECO is a clear borosilicate glass of high chemical resistance, and R14 is an epoxy resin. Further properties of these materials are set forth in Table VII below. Other lens materials may be used for some implementations.

TABLE-US-00007 TABLE VII Thermal coefficient of Index of Index of Index of expansion refraction refraction refraction Material (CTE) * 10E6 (at 20 C.) (at 60 C.) (at 100 C.) R14 66.00000000 1.50454192 1.49980491 1.49505707 D263TECO 7.20000000 1.51365480 1.51370440 1.51374334

[0032] For a particular implementation, the diffractive/refractive surface (i.e., Surface ID 10) of the hybrid lens B is can have characteristics as shown in FIG. 4, which indicates how phase and line frequency change with radius/distance from the center of the aperture. The curve 102 indicates the change in phase, whereas the curve 104 indicates the change in line frequency. Further, although the diffraction order of the hybrid diffractive/refractive surfaces described above is equal to four, in other implementations the diffraction order can be equal to one or another value. In general, the diffraction order may depend on the ease of manufacturing and/or the diameter of the hybrid diffractive/refractive lens B.

[0033] For the values of index of refraction, the computer modeling assumed that the index data is relative to air at the system temperature and pressure and that wavelengths are measured in air at the system temperature and pressure. For a wavelength of 0.940000 m, the absolute air index values were 1.000270 at 20 C., 1.000237 at 60 C., and 1.000212 at 100 C.

[0034] The foregoing details are illustrative only, and various properties or parameters of one or more of the lenses and lens surfaces can be adjusted in other implementations so as to obtain a substantially athermal optical assembly. For example, some parameters of the described implementations can be additionally described in terms of effective-focal-length normalized parameters such as in Table 8 below:

TABLE-US-00008 TABLE VIII Surface ID Type Radius Thickness Glass Diameter Conic Comment OBJ STANDARD Infinity 133.3274 32.50158 0 1 STANDARD Infinity 0.046665 D263TECO 0.489329 0 2 STANDARD Infinity 0.004444 R14 0.481951 0 STO STANDARD Infinity 0.011111 0.454578 0 4 EVENASPH 9.20796 0.064366 R14 0.488867 0 lens A 6 STANDARD Infinity 0.002222 R14 0.484804 0 base layer 7 STANDARD Infinity 0.066664 D263TECO 0.485298 0 wafer AB 8 STANDARD Infinity 0.002222 R14 0.500023 0 base layer 9 STANDARD Infinity 0.013028 R14 0.500517 0 10 BINARY_2 2.84781 0 0.488867 0 lens B defined by 12 STANDARD Infinity 1.048235 0.503204 0 glass 13 EVENASPH 0.33728 0.066664 R14 0.349943 0 lens C 14 STANDARD Infinity 0.002222 R14 0.3389 0 base layer 15 STANDARD Infinity 0.066664 D263TECO 0.337827 0 wafer CD 16 STANDARD Infinity 0.002222 R14 0.305866 0 base layer 17 STANDARD Infinity 0.008888 R14 0.304793 0 18 EVENASPH 0.78437 0.066664 0.293334 0 lens D 19 STANDARD Infinity 0 0.274356 0 IMA STANDARD Infinity 0 0.24769 0 VCSEL array

[0035] The described implementations can be additionally described in terms of an aspect ratio where the aspect ratio is defined as the largest diameter optical surface divided by the total track length of the hybrid optical assembly. For example, in some implementations the aspect ratio of the hybrid optical assembly can be 0.5, while in other implementations that aspect ratio can be larger or smaller depending on the intended application of the hybrid optical assembly. For example, for some implementations with a total track length about 4 mm, the aspect ratio can be about 0.356, while for some other implementations with a total track length of about 6.356 the aspect ratio can be about 0.224.

[0036] As indicated previously, the optical assembly 22 can be integrated as part of an optical pattern generator arranged to project an array or other pattern of dots onto a projection plane 36. As illustrated in the graphs of FIGS. 5A, 5B and 5C based on computer modeling, the optical assembly 22 can be used to project a high-quality array of dots onto the projection plane. In FIGS. 5A-5C, each curve (e.g., 202, 204) represents a different field point, for example, a projected dot from the VCSEL array 22. The values above the top of the graph (i.e., 0.000 mm-0.550 mm) indicate the distance of each field point from the center of the VCSEL array plane. FIG. 5A illustrates the curves at 20 C., FIG. 5B illustrates the curves at 60 C., and FIG. 5C illustrates the curves at 100 C.

[0037] Each curve in FIGS. 5A-5C indicates the fraction of the optical energy enclosed within a centroid having a given radius from the center of the dot projected onto the plane 36. The steepness of the slopes of the curves out to a radius of about 3.5 m is indicative of the high quality of the projected dots (i.e., most of the optical energy for each dot is contained within a centroid having a radius of about 3.5 m). Further, the high quality of the projected array of dots substantially is maintained over the temperature range of 20 C.-100 C. That is, at an operating temperature of about 20 C.-60 C., about 80% of light is enclosed in a circle (a dot) with a radius slightly less than about 3.4 m for all possible light source (VCSEL) positions, whereas up to an operating temperature of about 100 C., about 80% of light is enclosed in a circle with a radius slightly less than about 3.5 m for all possible light source (VCSEL) positions. Accordingly, the quality of the output of the athermal optical assembly 20 is substantially constant over the operating range 20 C. to 100 C. Thus, high quality system performance can be achieved even as the temperature varies.

[0038] Various modifications and combinations of features will be evident from the foregoing examples and are within the spirit of the invention. Accordingly, other implementations are within the scope of the claims.