The present application claims priority under 35 U.S.C. § 119 to DE 10 2018 208 897.7, filed in the Federal Republic of Germany on Jun. 6, 2018, the content of which is hereby incorporated by reference herein in its entirety.
The present invention relates to a receiving device for a lidar system. The present invention further relates to a method for manufacturing a receiving device for a lidar system.
Different variants of 3-D optoelectronic scanners are known. These are understood to include rotating macroscanners, MEMS-based scanners, OPA (optical phase array) lidar, and flash lidar. What all of the above-mentioned systems have in common is that they collect emitted laser light. In this context, there are optical systems that are made up of one lens or a plurality of lenses. What they all have in common is that they have a long optical receiving path, that is, a large number of lenses.
In this manner, a beam having a diameter in the centimeter range can be guided in the transmission path via the rotating macromirror. Using such systems, in which all of the components “rotate,” it is inherent to the system that a horizontal field of view (FOV) of 360° can advantageously be scanned.
An optical detection system, which is made up of a lens system and forms an image of and/or focuses incident light on individual receivers, is known, e.g., from DE 10 2012 006 869 A1.
EB 2 955 558 A1 describes a lens system, as is or that can be used in a lidar system, the lens system including at least seven lenses.
DE 10 2011 107 585 A1 likewise describes a single lens, which is used in a lidar system in order to receive and emit light.
Current imaging systems or objectives are made up mostly of only individual lenses, which are generally optically transparent to the wavelengths stipulated by the scanner, and whose surfaces are shaped in such a manner that, when they function individually or cooperate, they guide the incident light to, and form an image of it on, the detector.
Most of these known systems have a considerable overall length. They react sensitively to temperature changes as a function of the lens material used (e.g., glass or plastic) and the selection of the housing material, which means that the optical efficiency and imaging capability suffer. This often has a direct effect on the range and resolution of such scanners. These objectives have a high weight due to the lens material.
An object of the present invention is to provide improved receiving optics for a lidar system.
According to a first aspect, the present invention provides a receiving device for a lidar system, where the receiving device 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 of the lidar system is able to impinge upon the limiting device, the first refracting element and the two reflector elements are formed and aligned with each other in such a manner that the received beam of the lidar system is foldable in relation to an axis of the received optical beam and guidable onto the detector element.
Due to the fact that air is present between the reflector elements, this keeps the overall length of the receiving device low. In this manner, the entire receiving device can advantageously take up less space and consequently become lighter, as well. In this manner, the receiving optics are advantageously less sensitive to temperature fluctuations. In addition, the focal point is advantageously not shifted, which means that chromatic aberration of the receiving device is prevented to the greatest extent possible.
According to a second aspect, the object is achieved by a method of manufacturing a receiving device for a lidar system, including the steps of: providing a limiting device for limiting an angle of entrance of a received optical beam; providing two reflector elements; and providing a detector element, where the limiting device is formed such that a received beam can impinge upon it and the receiving device and the two reflector elements are formed and aligned with each other such that the received beam of the lidar system is foldable in relation to an axis of the received optical beam and guidable onto the detector element.
In an example embodiment of the receiving device, a first reflector element includes spherical and conical portions. In this manner, from a standpoint of production engineering, this allows the receiving device to be manufactured more easily and cost-effectively.
In an example embodiment of the receiving device, the first reflector element includes aspherical portions. In this manner, from a standpoint of production engineering, this allows the receiving device to be manufactured in a further improved manner.
In an example embodiment of the receiving device, the detector element is situated in a central, recessed region of the first reflector element. In this manner, a chromatic aberration of the receiving device can advantageously be eliminated to the greatest extent possible; spots always being imaged identically, substantially independently of the angle of arrival of the laser beam.
In an example embodiment of the receiving device, a second refracting element is situated in a central, recessed region of the first reflector element. In this manner, the imaging quality of the receiving device can again be increased markedly; in particular, this allows even smaller spot sizes to be achieved.
In an example embodiment of the receiving device, the second reflector element is situated on the limiting device. In this manner, a smaller spot radius can be produced over the entire field of view.
In an example embodiment of the receiving device, the reflector elements are formed as specularly reflecting surfaces. This provides technically simple options for manufacturing the reflector elements.
In an example embodiment of the receiving device, the reflector elements are formed as specularly reflecting surfaces on surfaces of the limiting device. In this manner, the receiving device is essentially made up of a single element, which simplifies an installation and adjustment operation considerably. Through this, a particularly low space requirement of the receiving device is advantageously achieved.
In an example embodiment of the receiving device, the specularly reflecting surfaces each has a band-pass filter element, in particular, an interference filter. In this manner, a narrow-band characteristic of the receiving device is supported, which means that interfering background light can be substantially eliminated.
In the following, the present invention, including further features and advantages, is described in detail in light of a number of figures, in which identical or functionally equivalent components have the same reference numerals. In particular, the figures are meant to clarify certain principles of the present invention and are not necessarily drawn true to scale.
Device features described follow analogously from corresponding method features described, and vice versa. This means, in particular, that features, technical advantages, and explanations regarding the receiving device for a lidar system follow analogously from corresponding explanations, features, and advantages of the method of manufacturing a receiving device for a lidar system, and vice versa.
A central idea of the present invention is, in particular, to provide improved receiving optics for a lidar system.
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.
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.
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.
This configuration allows an imaging quality (e.g., spot radius) to increase even further in comparison with the set-up of
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.
Therefore, receiving device 100 of
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 μm at a 4.5° object angle. In particular, the set-up of
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.
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.
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
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
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.
All of the optical systems portrayed in
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.
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.
Number | Date | Country | Kind |
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102018208897.7 | Jun 2018 | DE | national |