The present invention relates to a lidar sensor, especially for motor vehicles, having a light source, a movable deflection mirror for producing a scanning beam that sweeps across a monitored space by deflecting a light beam emitted by the light source, and having an optical receiver for detecting light reflected by an object hit by the scanning beam in the monitored space.
In driver assistance systems for motor vehicles, lidar sensors are used, inter alia, for sensing the traffic environment, for example, for locating vehicles driving ahead or other obstacles.
When working with conventional lidar sensors of the aforementioned type, the light beam produced by the light source, for example, a semiconductor laser, is slightly widened by an optical system, so that it has a beam diameter of 1-2 mm, for example. This beam is then deflected by the deflection mirror and directly forms the scanning beam for locating objects. The deflection mirror is moved oscillatingly in one or two dimension(s), so that the scanning beam sweeps across a specific angular range or—in the case of a two-dimensional movement of the deflection mirror—a specific solid angle range that defines the monitored space.
The small beam diameter makes it possible for a small-sized deflection mirror to be used whose moment of inertia is correspondingly small, so that the mirror mechanism is not overloaded even at high oscillation frequencies, allowing the monitored space to be scanned at a high frame rate.
It is disadvantageous, however, that relatively high absorption and scattering losses occur under dusty, rainy or snowy conditions because the beam diameter is relatively small in comparison to the scattering particles (for example, snowflakes). Thus, unfavorable conditions limit the range and sensitivity of the lidar sensor. Moreover, the maximum permissible intensity of the laser beam is also limited by eye safety requirements. This also results in range and sensitivity restrictions.
As alternatives, what are generally referred to as macro scanning devices are available, where the optical system widens the laser beam to a significantly greater degree. In such situations, a very small beam angle of the scanning beam can be achieved in the far field because the beam parameter product is maintained. However, a very large dimensioned deflection mirror is needed to deflect the beam. As a whole, therefore, the lidar sensor is mostly tilted azimuthally. However, in such situations, the dimensions and mass inertia of the sensor allow only relatively small beam angles relative to the monitored space and/or low sampling frequencies and thus low frame rates. When an elevation angular resolution is also needed, multi-beam systems are mostly used, where a plurality of scanning beams are emitted at different elevation angles.
It is an object of the present invention to provide a lidar sensor that renders possible a high sampling frequency and/or a large beam angle relative to the monitored space in consideration of the required level of eye safety and low sensitivity to scattering particles.
This objective may be achieved in accordance with the present invention in that the light source and the deflection mirror are adapted for using the deflected light beam to scan an array of micro-optical elements, each one of which, in response to being impinged upon by this light beam, is widened into a divergent beam. Also, a light-concentrating element is configured at a distance from the array of micro-optical elements. It transforms the divergent beam into a beam which forms the scanning beam and whose beam diameter is larger than that of the deflected beam.
Together, the micro-optical elements and the light-concentrating element widen the beam in a manner similar to that of a macro scanning device, making it possible to ensure eye safety, even at elevated total power levels of the laser beam, since the beam diameter is larger than the pupil diameter of the human eye. Also, the sensitivity to scattering particles is just as low as that of macro scanning devices. However, since the beam that is incident to the deflection mirror has a substantially smaller diameter, a smaller-sized deflection mirror may be used that allows suitably high sampling frequencies. The beam that is deflected by the deflection mirror does not directly scan the monitored space, rather only the array of micro-optical elements. The direction in which the scanning beam is then emitted is a function of the position of that micro-optical element which is impinged upon relative to the optical axis of the light-concentrating element. Therefore, the beam angle relative to the monitored space may be appreciably larger than the angle through which the light beam is maximally deflected by the deflection mirror. This makes it possible for a monitored space to be scanned using a wide beam angle at a high frame rate.
Advantageous embodiments and refinements of the present invention are described herein.
The micro-optical elements may optionally be refractive elements (for example, diverging lenses) or reflecting elements (for example, convex or concave mirrors). Also, diffractive elements (for example, DOEs, diffractive optical elements) may be used.
The light-concentrating element may be an optical lens, in whose focal plane lies the array of micro-optical elements, so that the divergent beams are transformed by the lens into virtually parallel beams. Alternatively, a concave mirror would also be conceivable instead of a lens.
The light-concentrating element may simultaneously form the compound lens of the optical receiver, so that the arriving beam reflected by the object is coaxial with the emitted beam, eliminating the need for considering parallax errors in the analysis of the detected signal. For example, a beam splitter that deflects the received light onto a detector array may be provided in the optical path between the light source and the light-concentrating element, thus between the light source and the deflection mirror, between the deflection mirror and the array of micro-optical elements, or between the array of micro-optical elements and the light-concentrating element. In an embodiment, the array of micro-optical elements may also simultaneously function as a beam splitter.
To compensate for aberrations, a convex form may be advantageous for the array of micro-optical elements or for a mirror that deflects the light onto this array.
Exemplary embodiments of the present invention are described below with reference to the figures.
Lidar sensor 10 shown in
Deflection mirror 18 is pivotable about an axis 24 that extends orthogonally to the drawing plane in
The distance between array 20 and lens 30 corresponds approximately to the focal length of lens 30, so that the lens transforms divergent beam 28 into a virtually parallel beam of rays that lidar sensor 10 emits as a scanning beam 32. The emission direction of scanning beam 32 is thereby a function of the location of that micro-optical element 22 which is impinged upon at that instant by deflected beam 26. In this way, deflection mirror 18 also indirectly effects a deflection of scanning beam 32.
In the example shown in
In the configuration shown in
In the case of a one-dimensional lidar sensor, scanning beam 32 is only rotated in one dimension, for example, azimuthally, as shown in
On the other hand, in the case of a two-dimensional lidar sensor, where scanning beam 32 is also rotated in elevation, array 20 is a two-dimensional array that also extends orthogonally to the drawing plane in
In a practical example, light beam 14 produced by light source 12 has a diffraction index M2 of approximately 3.3, a beam angle of approximately 1.7°, and a diameter of approximately 0.14 mm at the thinnest point. Imaging lens 16 has a diameter of 3 mm and a focal length of 29 mm; the distance to the light source is 76 mm. Deflection mirror 18 is approximately 11 mm distant from imaging lens 16 and approximately 40 mm from array 20 of the micro-optical elements. In the main scanning direction (vertically in
As a further exemplary embodiment,
In this exemplary embodiment, lens 30 simultaneously forms the compound lens of a receiver 42a, which, in turn, has a beam splitter 50, for example, a partially reflecting mirror, that transmits the divergent beam from micro-optical elements 22a to lens 30, but deflects a portion of the received light to an image sensor 46a. It is self-evident that this configuration of receiver 42a is also possible in embodiments that include refractive elements as micro-optical elements; conversely, a receiver that is configured separately from lens 30, is also possible in combination with reflecting micro-optical elements 22a.
Provided in this example between deflection mirror 18 and array 20c is another mirror 52 that deflects the light to impinge along the optical axis of lens 30 onto array 20c.
As a modified exemplary embodiment,
Finally,
Number | Date | Country | Kind |
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102015217908.7 | Sep 2015 | DE | national |
Filing Document | Filing Date | Country | Kind |
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PCT/EP2016/067734 | 7/26/2016 | WO | 00 |
Publishing Document | Publishing Date | Country | Kind |
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WO2017/045816 | 3/23/2017 | WO | A |
Number | Name | Date | Kind |
---|---|---|---|
9285477 | Smith | Mar 2016 | B1 |
9360665 | Azuma | Jun 2016 | B2 |
10025082 | Shroff | Jul 2018 | B2 |
20040114250 | Kato | Jun 2004 | A1 |
20050264867 | Cho | Dec 2005 | A1 |
20070057211 | Bahlnnan | Mar 2007 | A1 |
20070146869 | Lauer | Jun 2007 | A1 |
20070195294 | Willey | Aug 2007 | A1 |
20080048936 | Powell | Feb 2008 | A1 |
20080094607 | Bernard et al. | Apr 2008 | A1 |
20120051383 | Stern | Mar 2012 | A1 |
20140071431 | Last | Mar 2014 | A1 |
20140192406 | Bathe | Jul 2014 | A1 |
20150176977 | Abele | Jun 2015 | A1 |
20150234178 | Azuma | Aug 2015 | A1 |
20150355449 | Orth | Dec 2015 | A1 |
20170010473 | Ide | Jan 2017 | A1 |
Number | Date | Country |
---|---|---|
102011007243 | Oct 2012 | DE |
2110699 | Oct 2009 | EP |
H1096624 | Apr 1998 | JP |
2010505631 | Feb 2010 | JP |
2011191633 | Sep 2011 | JP |
2012237810 | Dec 2012 | JP |
2013125165 | Jun 2013 | JP |
2015114562 | Jun 2015 | JP |
2015532462 | Nov 2015 | JP |
2016040630 | Mar 2016 | JP |
Entry |
---|
International Search Report dated Oct. 13, 2016, of the corresponding International Application PCT/EP2016/067734 filed Jul. 26, 2016. |
Number | Date | Country | |
---|---|---|---|
20180267148 A1 | Sep 2018 | US |