RECEIVING DEVICE FOR A LIDAR SYSTEM
20190377069 ยท 2019-12-12
Inventors
Cpc classification
G02B17/061
PHYSICS
G01S17/42
PHYSICS
G02B17/086
PHYSICS
International classification
Abstract
A receiving device for a lidar system includes: a limiting device for limiting an angle of entrance of a received optical beam; two reflector elements; and a detector element, where the received optical beam can impinge upon the limiting device and the first refracting element and the two reflector elements are formed and aligned with each other such that the received beam is foldable in relation to an axis of the received optical beam and guidable onto the detector element.
Claims
1. A receiving device for a lidar system, the receiving device comprising: an optical limiter, wherein the optical limiter is designed for limiting an angle of entrance of a received optical beam; a first reflector; a second reflector; and a detector; wherein: the optical limiter is arranged so that the received optical beam of the lidar system is able to impinge upon the optical limiter; and the optical limiter and the reflectors are aligned relative to one another to fold the received optical beam onto the detector.
2. The receiving device of claim 1, wherein the first reflector includes spherical and conical portions.
3. The receiving device of claim 2, wherein the first reflector includes aspherical portions.
4. The receiving device of claim 2, wherein the detector is situated in a central recessed region of the first reflector.
5. The receiving device of claim 2, wherein a refractor is situated in a central recessed region of the first reflector.
6. The receiving device of claim 1, wherein the second reflector is situated on the optical limiter.
7. The receiving device of claim 1, wherein the reflectors include as specularly reflecting surfaces.
8. The receiving device of claim 7, wherein the specularly reflecting surfaces each includes a band-pass filter.
9. The receiving device of claim 8, wherein band-pass filter is an interference filter.
10. The receiving device of claim 1, wherein the reflectors include specularly reflecting surfaces and are formed on surfaces of the optical limiter.
11. A method of manufacturing a receiving device for a lidar system, the method comprising: providing an optical limiter for limiting an angle of entrance of a received optical beam that impinges upon the optical limiter; providing a first reflector and a second reflector; aligning the optical limiter and the reflectors relative to one another to fold the received optical beam onto the detector.
12. A 3-D optoelectronic scanner comprising a lidar system, the lidar system including a receiving device, the receiving device comprising: an optical limiter, wherein the optical limiter is designed for limiting an angle of entrance of a received optical beam; a first reflector; a second reflector; and a detector; wherein: the optical limiter is arranged so that the received optical beam of the lidar system is able to impinge upon the optical limiter; and the optical limiter and the reflectors are aligned relative to one another to fold the received optical beam onto the detector.
Description
BRIEF DESCRIPTION OF THE DRAWING
[0024]
[0025]
[0026]
[0027]
[0028]
[0029]
DETAILED DESCRIPTION
[0030] A central idea of the present invention is, in particular, to provide improved receiving optics for a lidar system.
[0031] A receiving device for, e.g., a 3-D optoelectronic scanner having specularly reflecting surfaces is provided, the specularly reflecting surfaces being able to be produced, for example, by depositing metal (e.g., in the form of silver, aluminum, gold, etc.). In addition, by optionally depositing a dielectric layer on the specularly reflecting surfaces, a wavelength-selective mirror can be produced, which can act simultaneously as an optical filter in the 3-D scanner and help to suppress or minimize interfering background light.
[0032] Due to this, the medium that fills the space between the mirrors is air. However, there is the option of filling up this space with another optically transparent medium (e.g., glasses, such as BK7; plastics, such as polycarbonate, zeonex, etc.; liquids, such as oils). In this last-mentioned, monolithic set-up, the boundary surfaces are plated with the above-mentioned, specularly reflecting layers, so that these have reflecting characteristics for the corresponding wavelengths. In this context, the entrance surfaces themselves of this monolith can have optical beam-shaping characteristics. An advantage of such a set-up is an extremely compact design of the receiving device.
[0033]
[0034] The surfaces of reflector elements 10, 11 are spherical and can include an additional conical portion. Also, the surfaces of reflector elements 10, 11 can optionally include aspherical portions. Detector element 20 can take the form of a 0-D (single-pixel) detector, 1-D array or 2-D array detector (CCD, CMOS imager, PIN diodes, APD (avalanche photodiode), SPAD (single photon avalanche diode), etc., which can be made up of one or more pixels. A plurality of 0-D detectors can also be arranged in an arbitrary pattern so as to have a particular spatial separation perpendicular to the beam direction.
[0035]
[0036] This configuration allows an imaging quality (e.g., spot radius) to increase even further in comparison with the set-up of
[0037]
[0038] The lens material of refracting elements 1, 30 is preferably made up of the material N-BK7, but any other lens material can also be used.
[0039]
[0040]
[0041] Therefore, receiving device 100 of
[0042] For all of the example embodiments mentioned above, an f-number lies, for example, in a range of approximately 1.15 to approximately 1.20, preferably in a range of approximately 1.16 to 1.18. A spot size of an image point increases from a few micrometers at a 0 object angle to approximately 1200 m at a 4.5 object angle. In particular, the set-up of
[0043] The proposed, reflector-based receiving devices 100 permit effective imaging within a FOV of 5, the FOV being able to be expanded by a combination of a plurality of these objectives, the individual objectives being able to be positioned at a suitable angle to each other, so that as a result, a greater FOV can be produced. In this case, the term objective stands for a reflector-based receiving device.
[0044] The proposed receiving devices can be used for biaxial and coaxial flash lidar; macroscanners, in which the receiving unit and/or transmitting unit are rotated along or only one rotating reflector deflects the transmitted and received laser light onto the static transmitting and receiving units; FMCW lidar; MEMS lidar; OPA lidar; etc.
[0045] Proposed receiving devices 100 are suited to different variants of 3-D optoelectronic scanners, as desired. If the resolution of the surrounding area is produced on the imager/detector, which is made up of a plurality of pixels (e.g., CCD, CMOS imagers, 2-D and line detectors, SPAD and APD), then the image point should range in the magnitude of the pixel size. In particular, receiving devices 100 of
[0046] If the spatial resolution is no longer generated on the receiving side, but, for example, using temporally staggered firing of laser light pulses, then, as a rule, larger pixels, on which a plurality of object points are imaged, are used, in this case, a poorer resolution of the lens systems being sufficient. Such a system is represented, for example, by receiving device 100 in
[0047] The proposed, reflector-based receiving devices 100 advantageously have a nearly constant imaging quality as a function of the wavelength and can therefore be adapted for different wavelengths without modification of the optical design.
[0048] All of the optical systems portrayed in
[0049]
[0050]
[0051] In summary, the present invention provides reflector systems that can be combined with lenses. In this manner, structurally smaller and lighter scanners can advantageously be produced, which are less sensitive to changes in the operating temperature.
[0052] It is clear to one skilled in the art that numerous modifications to the present invention are possible without departing from the essence of the invention.