LOW DIVERGENCE VERTICAL CAVITY SURFACE EMITTING LASERS, AND MODULES AND HOST DEVICES INCORPORATING THE SAME

Abstract

The disclosure describes VCSELs operable to produce very narrow divergent light beams. The narrow divergent beam can be obtained, in part, by incorporating an additional epitaxial layer so as to increase the cavity length of the VCSEL. The increased cavity length can result in higher power in fewer larger diameter transverse modes, which can significantly reduce the output beam divergence. The additional epitaxial layer can be incorporated, for example, into a top-emitting VCSEL or bottom-emitting VCSEL.

Claims

1. A vertical cavity surface emitting laser (VCSEL) comprising: a substrate; an epitaxial VCSEL structure on the substrate, wherein the epitaxial VCSEL structure includes: a resonant cavity, including a gain region, disposed between a bottom mirror and a partially reflecting middle mirror, the partially reflecting middle mirror being further from the substrate than the bottom mirror; and an additional epitaxial layer disposed between the partially reflecting middle mirror and a top mirror, the top mirror being further from the substrate than the partially reflecting middle mirror, and the additional epitaxial layer having a thickness in a range of 5 μm-100 μm.

2. The VCSEL of claim 1 wherein the additional epitaxial layer has a thickness in a range of 5 μm-50 μm.

3. The VCSEL of claim 1 wherein the top mirror is partially reflecting, and the VCSEL is operable as a top-emitting VCSEL to produce an output beam emitted through the top mirror.

4. The VCSEL of claim 1 wherein the bottom mirror is partially reflecting, and the VCSEL is operable as a bottom-emitting VCSEL to produce an output beam emitted through the bottom mirror.

5. The VCSEL of claim 1 wherein the VCSEL is operable to produce a light beam that is emitted from the VCSEL, the light beam having a full-width half-maximum beam divergence of no more than 10 degrees.

6. The VCSEL of claim 5 wherein the VCSEL is operable to produce a light beam that is emitted from the VCSEL, the light beam having a full-width half-maximum beam divergence in a range of 0.5-5 degrees.

7. The VCSEL of claim 1 including an aperture to concentrate current in a particular part of the gain region, wherein the partially reflecting middle mirror is disposed between the gain region and the additional epitaxial layer.

8. The VCSEL of claim 3 wherein the VCSEL is operable to produce a light beam that is emitted from the VCSEL, the additional epitaxial layer being transparent to a wavelength of the light beam, and the substrate being opaque to the wavelength of the light beam.

9. The VCSEL of claim 8 wherein the additional epitaxial layer is composed of AlGaAs, and the substrate is composed of GaAs.

10. The VCSEL of claim 8 wherein the substrate is composed of GaAs, and the additional epitaxial layer is transparent to a wavelength less than 950 nm.

11. A vertical cavity surface emitting laser (VCSEL) comprising: a substrate; an epitaxial VCSEL structure on the substrate, wherein the epitaxial VCSEL structure includes: a resonant cavity, including a gain region, disposed between a top mirror and a partially reflecting middle mirror, the top mirror being further from the substrate than the partially reflecting middle mirror; and an additional epitaxial layer disposed between the partially reflecting middle mirror and a bottom mirror, the partially reflecting middle mirror being further from the substrate than the bottom mirror, and the additional epitaxial layer having a thickness in a range of 5 μm-100 μm.

12. (canceled)

13. The VCSEL of claim 11 wherein the top mirror is partially reflecting, and the VCSEL is operable as a top-emitting VCSEL to produce an output beam emitted through the top mirror.

14. The VCSEL of claim 11 wherein the bottom mirror is partially reflecting, and the VCSEL is operable as a bottom-emitting VCSEL to produce an output beam emitted through the bottom mirror.

15.-20. (canceled)

21. The VCSEL of claim 1 wherein the gain region includes a plurality of stacked quantum well groups separated from one another by one or more tunnel junctions.

22. A VCSEL array comprising: a plurality of VCSELs in accordance with claim 1; and a plurality of contacts each of which is electrically connected to one or more of the VCSELs.

23. The VCSEL array of claim 22 wherein the VCSELs are arranged in a regular pattern.

24. The VCSEL array of claim 22 wherein the VCSELs are in a random arrangement.

25. An optical sensor module comprising: an optical source including a VCSEL according to claim 1, the VCSEL being operable to generate a narrow divergence source beam directed through a window toward an object; an optical detector to sense light reflected back from the object illuminated by the narrow divergence source beam; and a computation device operable to determine a distance to the object or a physical characteristic of the object based at least in part on a signal from the optical detector.

26. A host device comprising an optical sensor module according to claim 25, wherein the host device is operable to use data obtained by the optical detector of the optical sensor module for one or more functions executed by the host device.

27. The host device of claim 26 wherein the host device is a smart phone.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0017] FIG. 1 illustrates a top-emitting VCSEL structure.

[0018] FIG. 2 illustrates another top-emitting VCSEL structure.

[0019] FIG. 3 illustrates a further top-emitting structure.

[0020] FIG. 4 illustrates a bottom-emitting VCSEL structure.

[0021] FIG. 5 illustrates another bottom-emitting VCSEL structure.

[0022] FIGS. 6A and 6B illustrate examples of VCSEL arrays.

[0023] FIG. 7 illustrates an example of a proximity sensor module that includes a low beam divergence VCSEL.

[0024] FIG. 8 illustrates an example of a host device that includes a low beam divergence VCSEL.

DETAILED DESCRIPTION

[0025] As shown in FIG. 1, a top-emitting VCSEL device 20 includes a VCSEL structure grown epitaxially on a substrate 22. The VCSEL resonant cavity is formed between a first lower mirror 24 and a second upper mirror 26. The bottom mirror 24 can be implemented, for example, as high-reflectivity distributed Bragg reflector (DBR). The top mirror 26, which can be implemented, for example, as a DBR or as a multi-layer dielectric coating, has a lower reflectivity such that it is only partially reflecting, thereby allowing an output beam 36 to exit through the top of the VCSEL (i.e., through the end of the VCSEL 20 furthest from the substrate 22). A laser gain region 28 comprising a stack or group of multiple quantum wells is disposed between the mirrors 24, 26. The gain (i.e., active) region 28 is activated by a current flowing between top and bottom contacts (e.g., electrodes) 30, 32. In some designs, the quantum wells in the gain region 28 are activated by shining a laser beam on them to pump the carriers optically. In a VCSEL activated by current, an aperture 34 can be used to concentrate the current in the center region. This aperture 34 can be formed, for example, by oxidation, although other techniques such as ion implantation can be used to form the electrically insulating region around the aperture. The high gain results in laser oscillation between the mirrors 24, 26.

[0026] The VCSEL device 20 preferably also includes a third (middle) mirror 27 disposed between the gain region 28 and the top mirror 26. Thus, the VCSEL cavity is a 3-mirror cavity. The middle mirror 27 can be implemented, for example, as a DBR. The reflectivity of the middle mirror 27 should be designed such that the middle mirror by itself (i.e., in the absence of the top mirror 26) is insufficient to achieve lasing, the combined reflectivity of the middle mirror 27 and the top mirror 26 allows the VCSEL 20 to achieve lasing.

[0027] An epitaxial layer 38 is disposed between the middle mirror 27 and the top mirror 26 such that both the middle mirror 27 and the epitaxial layer 38 are disposed between the gain region 28 and the top mirror 26. As illustrated in the example of FIG. 1, the epitaxial layer 38 can be sandwiched between the middle mirror 27 and the top mirror 26 such that the epitaxial layer 38 is in direct contact with both the middle mirror 27 and the top mirror 26. The addition of the epitaxial layer 38 can help reduce the divergence of the output beam 36. Preferably, the epitaxial layer 38 is made relatively thick (e.g., 5 μm-25 μm; and, in some cases, even thicker, such as up to 50 μm or even up to 100 μm). In some instances, the epitaxial layer 38 has a thickness of about 25 μm. Other thicknesses may be appropriate for some implementations.

[0028] In some implementations, the epitaxial layer 38 is composed of a semiconductor material that is transparent to at least some wavelengths for which the substrate 22 is opaque. For example, in some implementations, the substrate 22 is composed of gallium arsenide (GaAs), and the epitaxial layer 38 is composed of aluminum gallium arsenide (AlGaAs). In such cases, the alloy composition (e.g., the percentage of aluminum) of the epitaxial layer 38 can be controlled such that the AlGaAs layer has a particular band gap that renders the AlGaAs layer transparent to wavelength(s) of light produced by the VCSEL. This allows the VCSEL to be tailored to emit relatively short wavelengths of light (e.g., less than 950 nm), even though the GaAs substrate 22 is opaque to such wavelengths.

[0029] The present techniques can be applied, for example, to top emitting VCSELs and, as noted above, can be used advantageously for VCSELs operable to emit light of shorter wavelengths (e.g., <950 nm). In some implementations, the epitaxial layer 38 is composed of other semiconductor compounds that are substantially lattice matched to the adjacent semiconductor material(s). For example, in some cases, the epitaxial layer 38 is composed of InGaAsP, GaN, or GaAsP including ZnSe.

[0030] FIG. 2 illustrates another example of a VCSEL device 20A which is similar to FIG. 1, except that the thick epitaxial layer 38 is grown closer to the bottom side of the VCSEL cavity. As shown in FIG. 2, the epitaxial layer 38 is disposed between, and in contact with, the bottom mirror 24 and the middle mirror 27, all of which are disposed between the substrate 22 and the gain region 28. The epitaxial layer 28 of FIG. 2 can have a similar thickness and composition as described above in connection with the VCSEL device of FIG. 1. Placing the gain region 28 closer to the top (i.e., light emitting) surface of the VCSEL device can be advantageous in some cases. For example, the output beam 36 can have a smaller diameter.

[0031] The present techniques for reducing divergence of the VCSEL output beam can be combined with other techniques that help reduce the divergence. For example, in some instances, the gain region 28 can be increased in length by using multiple gain sections instead of just a single gain section group of multiple quantum wells. The gain sections can be separated from one another by tunnel junction(s), with each gain section being placed at the maximum intensity point of the resonant cavity standing wave so that the cavity length increases in half wavelengths by the number of added gain sections. The resulting VCSEL device can have a lower divergent beam because of the longer cavity, and also can have higher intensity because of the higher gain from the multiple gain sections. An example is illustrated in FIG. 3, which shows a VCSEL device 20B similar to that of FIG. 1, but whose gain region 28 includes multiple quantum well groups 40 separated by a tunnel junction 42. Such stacked gain regions can, in some cases, produce higher gain so as to produce higher output power and efficiency, and may also reduce capacitance for higher modulation frequency. The foregoing feature of a gain region having multiple stacked gain sections can be incorporated into any of the implementations described in this disclosure, including those described below.

[0032] Further, in some cases, the cavity length can be extended by increasing the number of DBR mirrors in a stack for the bottom mirror 24 (or the top mirror 26). For example, in GaAs/GaAlAs DBRs, reducing the Al concentration will need a larger number of mirror pairs for a particular reflectivity, thereby increasing the cavity length. The increase in cavity length will reduce the number of higher order modes and will thus reduce the divergence angle. In some instances, the DBR mirror stack includes multiple DBR mirror pairs composed of alternating layers of different materials having a refractive index difference in a range of 1-7%. The foregoing features can be incorporated into any of the implementations described in this disclosure, including those described below.

[0033] The addition of a relatively thick epitaxial layer also can be incorporated into bottom-emitting VCSEL structures. FIGS. 4 and 5 illustrate examples of such VCSEL devices. In FIGS. 4 and 5, each of the bottom and middle mirrors 24, 27 is partially reflecting, and the beam 36 is emitted from the VCSEL device through the GaAs or other substrate 22. As shown in FIG. 4, the VCSEL device 20D includes an epitaxial layer 38 disposed between the middle mirror 27 and the top mirror 26. Both the middle mirror 27 and the epitaxial layer 38 are disposed between the gain region 28 and the top mirror 26. On the other hand, as shown in FIG. 5, the VCSEL device 20E includes an epitaxial layer 38 disposed between the bottom mirror 24 and the middle mirror 27. In this implementation, both the bottom mirror 24 and the middle mirror 27, as well as the epitaxial layer 38, are disposed between the substrate 22 and the gain region 28. The epitaxial layers 28 of FIGS. 4 and 5 can have a similar thickness and composition as described above in connection with the VCSEL device of FIG. 1.

[0034] Bottom emitting VCSELs sometime operate to emit longer wavelengths, with respect to which the substrate 22 is transparent. An advantage that can be achieved in some instances (e.g., the VCSEL device 20D of FIG. 4) is better cooling because a heat sink can be placed on the top contact 30, closer to the VCSEL structure. Further, in the example of FIG. 5, the thick epitaxial layer 38 is grown on the bottom side of the VCSEL cavity such that the gain region 38 is closer to the top surface of the VCSEL device. This can result in even better cooling of the gain region 38 in some situations.

[0035] In each of the foregoing implementations, the additional epitaxial layer 38 is composed of a semiconductor material (e.g., a semiconductor compound) whose composition differs from that of the adjacent mirror structures.

[0036] Multiple VCSELs, each of which has an additional epitaxially grown layer as described above, can be integrated into a VCSEL array. For example, the VCSELs 50 in the array may be regularly spaced so that they are arranged in a regular pattern (FIG. 6A) or randomly spaced so that they are in a random arrangement (FIG. 6B). The VCSELs 50 can be connected by respective electrical connections 54 to respective electrical contacts 52 such that the VCSELs are addressable, and can be activated or deactivated, either individually or in groups.

[0037] FIG. 7 illustrates an example of a proximity sensor module that includes a low beam divergence VCSEL source such as one of those described above (e.g., FIG. 1, 2, 3, 4 or 5). The VCSEL 150 and a light detector (e.g., a photodetector) 151 are mounted close together on a common substrate 153. The VCSEL beam propagates out through a window 107 and reflects and scatters off an object outside the module. A portion of the backscatter radiation 108 returns through the window 107 and is captured by the detector 151. The signal intensity from the detector is used by processing circuitry to determine the distance of the object from the sensor. In the illustrated example, the VCSEL beam divergence is sufficiently small that the specular reflection 152 from the window 107 returns close to the VCSEL and does not fall on the detector 151. Thus, this reflection 152 does not add a noise signal to modify the backscatter signal received by the detector 151 and so does not degrade the distance determination.

[0038] The illustrated optical sensor module thus includes, as an optical source, a VCSEL device operable to generate a narrow divergence source beam directed through a window toward an object, the narrow divergence source beam having, in some cases, a full-width half-maximum beam divergence of no more than 10 degrees. The module further includes an optical detector to sense light reflected back from the object illuminated by the narrow divergence source beam, and a computation device 160 including processing circuitry operable to determine a distance to the object or a physical characteristic of the object based at least in part on a signal from the optical detector. The processing circuitry can be implemented, for example, as one or more integrated circuits in one or more semiconductor chips with appropriate digital logic and/or other hardware components (e.g., read-out registers; amplifiers; analog-to-digital converters; clock drivers; timing logic; signal processing circuitry; and/or microprocessor). The processing circuitry is, thus, configured to implement the various functions associated with such circuitry.

[0039] Some implementations provide narrower divergent beams, for example, in the range of 0.5 to 5 degrees to provide much higher proximity sensing accuracy in a smaller footprint assembly.

[0040] Additional benefits can be obtained by using the low divergence beam from the VCSEL. The beam that impinges on the object is relatively small, thereby resulting in a higher incident power density. Therefore, the scattered and reflected power is proportionally higher. These features can result in improved distance measurement resolution with shorter pulses, as well as the ability to measure longer distances. These benefits can be accomplished in a small footprint since a small distance between the VCSEL and detector can be maintained.

[0041] The foregoing description is made in relation to proximity sensing of objects for applications such as self-focusing of cameras and other motion detection applications. However, other applications of the technology will be readily apparent. For example, the very low divergence VCSEL source beam also can be used for health monitoring by measuring, e.g., blood flow, heart pulse rate and/or chemical composition. In these applications, the source beam is directed at the sample or object, and the detector measures quantity of reflected light at one or more wavelengths or fluctuation of reflected light which correlates with pulsing effects from a heart-beat. It can be equally important in these other applications for the VCSEL to have the same very low divergence properties described above. The sensitivity of these applications likewise can be improved by incorporating the technology of this disclosure. The present technology also can be useful, for example, for other optical sensing modules, such as for gesture sensing or recognition.

[0042] VCSELs as described above, or modules incorporating one or more such VCSELs, can be integrated into a wide range of host devices such as smartphones, laptops, wearable devices, other computers, and automobiles. The host devices may include processors and other electronic components, and other supplemental modules configured to collect data, such as cameras, time-of-flight imagers. Other supplemental modules may be included such as ambient lighting, display screens, automotive headlamps, and the like. The host devices may further include non-volatile memory where instructions for operating the optoelectronic modules, and in some instances the supplemental modules, are stored.

[0043] FIG. 8 illustrates a smartphone 270 as an example of a host device that includes a module for three-dimensional optical imaging and/or sensing. The module is operable to emit light and to detect incoming beams. The module includes a VCSEL light source 274 operable to produce a very low divergence beam as described above. The module further includes a sensor 276 operable to sense incoming beams. The VCSEL light source 274 and the sensor 276 can be mounted, for example, on a printed circuit board or other substrate 278. The module also can include projection optics 279A and/or collection optics 279B, which can be implemented, for example, as lenses or other passive optical elements. Signal processing circuitry is operable to process signals detected by the sensor 276 and to determine, for example, the distance to an object outside the smartphone 270 that reflects some of the light back toward the smartphone, and/or for gesture recognition.

[0044] As modules using the VCSELs described above can obtain more accurate data in some cases, and the data can be used for functions executed by the smartphones (e.g., screen response to user proximity), these and other functions can be more accurately performed, thereby conferring substantial advantages to the smartphone or other host device itself.

[0045] In some cases, multiple VCSELs, as described above, can be incorporated into an array of VCSELs. In some implementations, one or more VCSELs are arranged in a module operable to produce structured light.

[0046] Although a broad framework of the disclosure is described with reference to a few preferred embodiments, other implementations may be configured by applying combinations and sub-combinations of elements described in this disclosure. Accordingly, other implementations are within the scope of the claims.