CN111175769A - Off-axis scanning distance measuring system - Google Patents

Off-axis scanning distance measuring system Download PDF

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Publication number
CN111175769A
CN111175769A CN202010093833.2A CN202010093833A CN111175769A CN 111175769 A CN111175769 A CN 111175769A CN 202010093833 A CN202010093833 A CN 202010093833A CN 111175769 A CN111175769 A CN 111175769A
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China
Prior art keywords
light beam
polarized light
liquid crystal
incident
pixel unit
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CN202010093833.2A
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Chinese (zh)
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CN111175769B (en
Inventor
关健
徐松
朱亮
闫敏
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Shenzhen Oradar Technology Co Ltd
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Shenzhen Oradar Technology Co Ltd
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Priority to CN202010093833.2A priority Critical patent/CN111175769B/en
Publication of CN111175769A publication Critical patent/CN111175769A/en
Priority to PCT/CN2020/141283 priority patent/WO2021159883A1/en
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    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01S—RADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S17/00—Systems using the reflection or reradiation of electromagnetic waves other than radio waves, e.g. lidar systems
    • G01S17/02—Systems using the reflection of electromagnetic waves other than radio waves
    • G01S17/06—Systems determining position data of a target
    • G01S17/08—Systems determining position data of a target for measuring distance only
    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01S—RADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S17/00—Systems using the reflection or reradiation of electromagnetic waves other than radio waves, e.g. lidar systems
    • G01S17/88—Lidar systems specially adapted for specific applications
    • G01S17/89—Lidar systems specially adapted for specific applications for mapping or imaging
    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01S—RADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S7/00—Details of systems according to groups G01S13/00, G01S15/00, G01S17/00
    • G01S7/48—Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S17/00
    • G01S7/481—Constructional features, e.g. arrangements of optical elements
    • G01S7/4814—Constructional features, e.g. arrangements of optical elements of transmitters alone
    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01S—RADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S7/00—Details of systems according to groups G01S13/00, G01S15/00, G01S17/00
    • G01S7/48—Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S17/00
    • G01S7/481—Constructional features, e.g. arrangements of optical elements
    • G01S7/4816—Constructional features, e.g. arrangements of optical elements of receivers alone
    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01S—RADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S7/00—Details of systems according to groups G01S13/00, G01S15/00, G01S17/00
    • G01S7/48—Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S17/00
    • G01S7/481—Constructional features, e.g. arrangements of optical elements
    • G01S7/4817—Constructional features, e.g. arrangements of optical elements relating to scanning
    • G—PHYSICS
    • G02—OPTICS
    • G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B27/00—Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
    • G02B27/28—Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00 for polarising
    • G02B27/283—Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00 for polarising used for beam splitting or combining

Abstract

The invention discloses an off-axis scanning distance measuring system, which comprises a transmitter, a collector and a control and processing circuit, wherein the transmitter is connected with the collector; the transmitter comprises a light source, a beam shaping component and a first cascade liquid crystal polarization grating; the first cascade liquid crystal polarization grating is used for diffracting the light beam to generate a diffracted light beam, and the diffracted light beam irradiates the target to be detected and is reflected to obtain a reflected light beam; the collector comprises a pixel unit, an imaging lens unit, a polarization selection component and a second cascade liquid crystal polarization grating; the second cascade liquid crystal polarization grating is used for forming a circularly polarized light beam; the emitter and/or the collector are configured to enable the position of each polarized light beam formed after each circularly polarized light beam passes through the polarization selection component to be incident on the pixel unit in the overlapping area to correspond to each pixel in the pixel unit in a one-to-one mode. The invention effectively solves the problems of measurement errors and the like caused by overlapping of light spots on the pixel units.

Description

Off-axis scanning distance measuring system
Technical Field
The invention relates to the technical field of computers, in particular to an off-axis scanning distance measuring system.
Background
At present, a Time of Flight (Time of Flight) principle and a structured light (structured light) principle are utilized to measure a distance of a target so as to obtain a depth image containing a target depth value, and further, functions such as three-dimensional reconstruction, face recognition and man-machine interaction can be realized based on the depth image. Related distance measurement systems have been widely used in the fields of consumer electronics, unmanned driving, AR/VR, and the like. The distance measuring system based on the time-of-flight principle includes a light beam emitter and a collector, wherein a light source in the emitter emits a light beam towards a target space to provide illumination, and the light beam reflected by the target is received by the collector. Wherein the time-of-flight distance measuring system calculates the distance of the object by calculating the time required for the light beam to be received from emission to reflection; the structured light distance measuring system processes the reflected light beam pattern and calculates the distance of the object by using a trigonometry method.
According to the light path configuration between the emitter and the collector, the flight time distance measuring system can be divided into a coaxial mode and an off-axis mode; the coaxial system is generally that the emitter and the collector share one scanning device, such as an MEMS galvanometer, so that the scanning of a large field of view is realized; the off-axis distance measuring system usually does not need a scanning device, but more receiving elements (such as a pixel array) are arranged at the collector end, so that the distance of a plurality of points in a large field of view can be measured at one time.
Chinese patent application No. 201910990526.1 discloses an off-axis scanning system, which realizes the expansion of the field angle by configuring a cascade liquid crystal polarization grating in the scanning system, not only can expand a single field of view into two fields of view, but also can realize the scanning of the field of view by changing the diffraction angle of the cascade liquid crystal polarization grating; in addition, the selection and the collection of optical signals in two different fields of view are realized by arranging the polarization selection assembly.
The above background disclosure is only for the purpose of assisting understanding of the inventive concept and technical solutions of the present invention, and does not necessarily belong to the prior art of the present patent application, and should not be used for evaluating the novelty and inventive step of the present application in the case that there is no clear evidence that the above content is disclosed at the filing date of the present patent application.
Disclosure of Invention
It is an object of the present invention to provide an off-axis scanning distance measuring system to solve at least one of the above-mentioned problems of the background art.
In order to achieve the above purpose, the technical solution of the embodiment of the present invention is realized as follows:
an off-axis scanning distance measuring system comprises an emitter, a collector and a control and processing circuit; the emitter comprises a light source for emitting a light beam, a light beam shaping assembly for shaping the light beam and a first cascade liquid crystal polarization grating; the first cascade liquid crystal polarization grating is used for diffracting the shaped light beam to generate a first diffracted light beam and a second diffracted light beam with opposite polarization rotation directions, the first diffracted light beam and the second diffracted light beam irradiate a target to be detected, and a first reflected light beam and a second reflected light beam are obtained through reflection; the collector comprises a pixel unit, an imaging lens unit, a polarization selection component and a second-level liquid crystal polarization grating; the second cascade liquid crystal polarization grating is used for receiving and diffracting at least part of the first reflected light beam and at least part of the second reflected light beam reflected by the target so as to respectively form two beams of circularly polarized light beams with opposite polarization directions and different propagation directions; the circularly polarized light beams with the same rotation direction of the first reflected light beam and the second reflected light beam form an overlapping area on the pixel unit after passing through the polarization selection component and the imaging lens unit; the control and processing circuit is respectively connected with the emitter and the collector and is used for calculating the flight time between the emission and the collection of the light beam and calculating the distance of the target to be measured according to the flight time; the emitter and/or the collector are configured to enable the position of each polarized light beam formed after each circularly polarized light beam passes through the polarization selection component, which is incident on the pixel units in the overlapping area, to correspond to each pixel in the pixel units in a one-to-one mode.
In some embodiments, the first diffracted beam illuminates a first area on a target to be measured and reflects the first reflected beam; the second diffracted light beam irradiates a second area on the target to be detected and reflects the second reflected light beam; the first reflected light beam forms a first left-handed circularly polarized light beam and a first right-handed circularly polarized light beam which have different propagation directions after passing through the cascade liquid crystal polarization grating; and the second reflected light beam passes through the cascade liquid crystal polarization grating to form a second left-handed circularly polarized light beam and a second right-handed circularly polarized light beam with different propagation directions.
In some embodiments, the cascade liquid crystal polarization grating includes a plurality of layers of liquid crystal polarization gratings, and each layer of liquid crystal polarization grating is provided with a grating pitch and a grating line direction.
In some embodiments, the area of the overlap region is reduced to disappear by adjusting parameters configuring the off-axis scanning distance measurement system.
In some embodiments, the light source is an array light source, wherein the array of light sources is arranged such that the polarized light beams are incident on different pixel units in a non-coincident manner to form the overlapping region.
In some embodiments, a reticle is further included, the reticle being configured such that only one polarized beam is incident on the pixel unit when multiple polarized beams are incident on the same pixel unit.
In some embodiments, the parameters include one or more of design parameters of the cascaded liquid crystal polarization grating, an area of a light source incident on the cascaded liquid crystal polarization grating, an angle of a light source emission beam incident on the cascaded liquid crystal polarization grating, and a focal length of the imaging lens unit.
In some embodiments, a light source is used as a sample point, the light source is controlled to emit a light beam to be incident on the cascade liquid crystal polarization grating at a certain angle, the number of opened layers of the cascade liquid crystal polarization grating is adjusted to obtain a group of imaging light spots, and the arrangement mode of the light source array is designed according to the distribution relation of the imaging light spots on the pixel units; and repeating the design process by taking the added light sources as sample points.
In some embodiments, the mask is designed according to the space between light spots formed by the polarized light beams incident on the pixel units and the sizes of the light spots; and arranging the mask at the position where the polarized light beam transmitted along the opposite direction of the incident light path is incident on the pixel unit.
In some embodiments, the design parameters of the cascaded liquid crystal polarization grating include the pitch of a single layer of liquid crystal polarization grating and the grid line direction of each layer of liquid crystal polarization grating.
The technical scheme of the invention has the beneficial effects that:
compared with the prior art, the off-axis scanning distance measuring system can realize large-field measurement and effectively solve the problems of measurement errors and the like caused by overlapping of light spots on the pixel units.
Drawings
In order to more clearly illustrate the embodiments of the present invention or the technical solutions in the prior art, the drawings used in the description of the embodiments or the prior art will be briefly described below, and it is obvious that the drawings in the following description are only some embodiments of the present invention, and for those skilled in the art, other drawings can be obtained according to these drawings without creative efforts.
FIG. 1 is a schematic structural diagram of an off-axis scanning distance measuring system according to an embodiment of the present invention.
FIG. 2 is a schematic diagram of an off-axis scanning distance measurement in an embodiment of the invention.
Fig. 3a and 3b are schematic diagrams of a pixel unit according to an embodiment of the invention.
Fig. 4 is a schematic diagram of the reflected light beam of the first embodiment of the present invention being imaged on the pixel unit.
Fig. 5 is a diagram illustrating the reflected light beam forming an image on the pixel unit according to the second embodiment of the present invention.
Fig. 6 is a diagram illustrating an image formed by a reflected light beam on a pixel unit according to a third embodiment of the present invention.
Fig. 7 is a schematic structural diagram of a receiver according to a fourth embodiment of the present invention.
Fig. 8 is a diagram illustrating an image of a reflected light beam on a pixel unit according to a fourth embodiment of the present invention.
Detailed Description
In order to make the technical problems, technical solutions and advantageous effects to be solved by the embodiments of the present invention more clearly apparent, the present invention is further described in detail below with reference to the accompanying drawings and the embodiments. It should be understood that the specific embodiments described herein are merely illustrative of the invention and are not intended to limit the invention.
It will be understood that when an element is referred to as being "secured to" or "disposed on" another element, it can be directly on the other element or be indirectly on the other element. When an element is referred to as being "connected to" another element, it can be directly connected to the other element or be indirectly connected to the other element. The connection may be for fixation or for circuit connection.
It is to be understood that the terms "length," "width," "upper," "lower," "front," "rear," "left," "right," "vertical," "horizontal," "top," "bottom," "inner," "outer," and the like are used in an orientation or positional relationship indicated in the drawings for convenience in describing the embodiments of the present invention and to simplify the description, and are not intended to indicate or imply that the referenced device or element must have a particular orientation, be constructed in a particular orientation, and be in any way limiting of the present invention.
Furthermore, the terms "first", "second" and "first" are used for descriptive purposes only and are not to be construed as indicating or implying relative importance or implicitly indicating the number of technical features indicated. Thus, a feature defined as "first" or "second" may explicitly or implicitly include one or more of that feature. In the description of the embodiments of the present invention, "a plurality" means two or more unless specifically limited otherwise.
As an embodiment of the present invention, an off-axis scanning distance measuring system having a higher resolution or a larger field angle is provided. Referring to fig. 1, an off-axis scanning distance measuring system according to an embodiment of the present invention includes an emitter 11, a collector 12, and a control and processing circuit 10; wherein, emitter 11 provides emission light beam to target space, at least part of emission light beam forms reflection light beam after reflecting by object in space, at least part of light signal (photon) of reflection light beam is collected by collector 12; the control and processing circuit 10 is connected to the emitter 11 and the collector 12, respectively, and synchronizes the trigger signals of the emitter 11 and the collector 12 to calculate the time required for the light beam to be emitted from the emitter 11 and reflected back to the collector 12 for reception, i.e. the flight time t between the emitted light beam and the reflected light beam, according to which the distance D of the corresponding point on the object can be calculated by the following formula:
D＝c·t/2 (1)
where c is the speed of light.
The transmitter 11 includes a light source 111, a beam shaping component 112, and a first cascaded Liquid Crystal Polarization Grating (LCPG) 113.
The light source 111 may be a light source such as a Light Emitting Diode (LED), an Edge Emitting Laser (EEL), a Vertical Cavity Surface Emitting Laser (VCSEL), or an array light source composed of a plurality of light sources; preferably, the light source 111 is an array light source composed of a plurality of VCSEL light sources, each of which may be individually disposed or a VCSEL array light source chip formed by generating a plurality of VCSEL light sources on a single semiconductor substrate. The light beam emitted by the light source 111 may be visible light, infrared light, ultraviolet light, or the like. The polarization state of the light beam is linear polarization, or the light beam can be an unpolarized light beam, wherein the polarization direction of the linear polarization can be arbitrarily set according to needs.
The light source 111 emits a light beam outwards under the control of the control and processing circuit 10, for example, in an embodiment, the light source 111 emits a pulse light beam at a certain frequency (pulse period) under the control of the control and processing circuit 10, which can be used in Direct time of flight (Direct TOF) measurement, the frequency is set according to the measurement distance, for example, the frequency can be set to 1 MHz-100 MHz, and the measurement distance is several meters to several hundred meters. In one embodiment, the light source 111 emits an amplitude modulated continuous wave light beam, such as a sinusoidal or square wave continuous wave light beam, out under the control of the control and processing circuitry 10, which may be used in Indirect time of flight (infrared TOF) measurements. It will be appreciated that the light source 111 may be controlled to emit the associated light beam by controlling a part of the processing circuitry 10 or independently of controlling sub-circuits present with the processing circuitry 10, such as a pulse signal generator.
The beam shaping assembly 112 receives the light beam from the light source 111 and shapes the light beam optically, such as by diffraction, refraction, reflection, etc., and then emits the shaped light beam into space, such as a focused light beam, a flood light beam, a structured light beam, etc. The beam shaping component 112 may be one or a combination of more of lens (including a lens group composed of a plurality of single lenses), Diffractive Optical Element (DOE), Diffuser (Diffuser), super surface (Metasurface) Optical Element, Micro Lens Array (MLA), powell prism, mask plate, mirror, MEMS (Micro-Electro-Mechanical System) galvanometer, and the like.
The cascade LCPG113 comprises a plurality of layers of LCPGs, each layer of LCPG is provided with own grating pitch and grating line direction for diffracting incident light beams, and the change of the cascade LCPG113 in the scanning direction and the scanning angle can be realized through the design of each layer of grating. For example, in one embodiment, the grating grid line direction of each LCPG in the cascade LCPG113 is the same, and at this time, the cascade LCPG can implement one-dimensional beam scanning perpendicular to the grid line direction; in one embodiment, the cascaded LCPG113 includes LCPGs with different grating grid line directions, such as a first LCPG including a plurality of grating grid lines along an x-axis direction and a second LCPG including a plurality of grating grid lines along a y-axis direction, and the first LCPG and the second LCPG are respectively used for realizing y-direction scanning and x-direction scanning, so as to realize two-dimensional scanning, for example: there are 10 layers of LCPG cascades, wherein the optical axis of the 1 st to 5 th layers of LCPG is along the x-axis, and the optical axis of the 2 nd to 10 th layers of LCPG is along the y-axis; alternatively, the optical axes of the 1 st, 3 rd, 5 th, 7 th and 9 th layers of LCPG are along the x-axis, and the optical axes of the 2 nd, 4 th, 6 th, 8 th and 10 th layers of LCPG are along the y-axis, and the specific arrangement manner can be set according to actual needs, and is not particularly limited in the present invention.
After a light beam enters a single-layer LCPG at a certain angle, the light beam is deflected due to the diffraction effect of the LCPG, and the deflection angle is determined by a grating equation, namely:
d(sinθ-sinα)＝mλ (2)
in one embodiment, the grating periods of each single-layer LCPG of the cascade LCPGs can be set to be different from each other or set to be the same, so that diffraction of different angles can be realized by independently controlling the switches of each layer of LCPG, and further the multi-angle scanning effect can be realized.
A liquid crystal 1/2 waveplate may also be disposed in the cascaded LCPG113, such as in one embodiment, the cascaded LCPG113 that forms a one-dimensional beam sweep by overlapping the liquid crystal 1/2 waveplate with a single LCPG. The liquid crystal 1/2 wave plate has two working states, is a 1/2 wave plate when no saturation voltage is added, and can be understood as common glass when the saturation voltage is added. The handedness of the circularly polarized light between the single LCPGs can be switched by the liquid crystal 1/2 wave plate, and the scanning angle of the cascade LCPG is determined by the liquid crystal 1/2 wave plate and the LCPG. In an embodiment, the cascade LCPG for two-dimensional scanning may also be formed by alternately cascading a single LCPG with vertical gate lines and a liquid crystal 1/2 wave plate, for example, 10 single LCPG cascades, where the optical axes of the 1 st, 3 rd, 5 th, 7 th, and 9 th LCPGs are along the x-axis and the optical axes of the 2 nd, 4 th, 6 th, 8 th, and 10 th LCPGs are along the y-axis, a liquid crystal 1/2 wave plate may be placed between two adjacent single LCPGs, or a liquid crystal 1/2 wave plate may be placed before the first LCPG, and the specific arrangement mode may be set according to actual needs, which is not particularly limited in the embodiment of the present invention.
Cascaded LCPG113 receives the beam from beam shaping component 112 and diffracts it into two diffracted beams with opposite polarization rotations: a first diffracted beam 131, a second diffracted beam 132 (e.g., +1 order 131, -1 order 132). The light beams from the beam shaping component 112 can be single-point, multi-point, flood light, line light beams, and the like, and are all linearly polarized or unpolarized light beams, and the two-stage diffracted lights formed after diffraction are all circularly polarized lights with opposite polarization rotation directions, for example, the first diffracted light beam 131 is left-handed circularly polarized light, and the second diffracted light beam 132 is right-handed circularly polarized light, and the propagation direction of the ± 1-stage diffracted light beams is determined by the cascade LCPG. It should be noted that when the beam shaping assembly outputs multi-spot beams, the +1 order diffracted beam is not the only one, but the +1 order beam is one set of multi-spot beams and the-1 order beam is the other set of multi-spot beams. The simultaneously emitted +1 order beam 131 and-1 order beam 132 illuminate a first area and a second area on the target. For a single point beam, the first region and the second region are a single point.
Collector 12 includes a pixel unit 121, an imaging lens unit 122, a Polarization selection component 123, and a second cascaded Liquid Crystal Polarization Grating (LCPG) for receiving the light beam emitted from the part of the emitter reflected back from the target. In the embodiment of the present invention, the second cascade Liquid Crystal Polarization Grating (LCPG) is shared with the first cascade Liquid Crystal Polarization Grating (LCPG) 113, and hereinafter, for convenience, is collectively referred to as the cascade LCPG 113. Namely: in some embodiments, transmitter 11 and collector 12 share the same cascaded LCPG 113; in one embodiment, two LCPGs 113 may also be designed or fabricated on the same optic to reduce volume.
In some embodiments, the pixel unit 121 may be a single pixel or a pixel array composed of a plurality of pixels, and the pixels may be CMOS, CCD, APD, SPAD, or the like which can convert an optical signal into an electrical signal.
After the first diffracted beam and the second diffracted beam emitted by the emitter 11 are reflected by the target in the first area and the second area, at least a part of the first diffracted beam and the second diffracted beam are reflected to form a beam 133 and a beam 134, respectively, and then the beam 133 and the beam 134 are incident into the cascaded LCPG113 of the collector 12, and the beam 133 and the beam 134 are diffracted by the cascaded LCPG113 to form a first polarized beam and a second polarized beam with opposite polarization directions but the same propagation direction, and the first polarized beam and the second polarized beam are further collected by the pixel unit 121 after passing through the polarization selection component 123 and the imaging lens unit 122. Since the propagation directions of the first polarized light beam and the second polarized light beam are the same, the two polarized light beams are finally imaged on the same area of the pixel unit 121. In addition, dynamic scanning can be realized by changing the number of the opening layers of the cascaded LCPG113, for example, the first region and the second region are scanned in the horizontal or vertical direction respectively, and the size and the position of the pixel unit 121 of the collector 12 do not need to be changed, so that large-field scanning measurement is realized.
Because the first polarized light beam and the second polarized light beam have almost the same propagation direction, the first polarized light beam and the second polarized light beam can be imaged in the region of the same pixel unit, and when the first polarized light beam and the second polarized light beam are imaged synchronously, images are superimposed to generate errors, and for this purpose, the two polarized light beams are selected by the polarization selection component 123 to ensure that only a single polarized light beam passes through or the two polarized light beams are further separated at the same time, so as to ensure that the two polarized light beams can be synchronously acquired by different regions on the pixel unit, and finally, the acquisition of the first polarized light beam and the second polarized light beam can be respectively realized by the reasonable configuration of the polarization selection component.
FIG. 2 is a schematic diagram illustrating the principle of off-axis scanning distance measurement in an embodiment of the present invention. The light source emitting beam 201 passes through the cascaded LCPG113 to emit a first diffracted beam 202 and a second diffracted beam 203 to illuminate a first area and a second area on the object, and since the object to be measured is a diffuser, the beam reflected back at the illuminated area will not have polarization maintaining characteristics, and the first reflected beam 204 reflected back at the first area and the second reflected beam 205 reflected back at the second area are unpolarized reflected beams. The unpolarized reflected light beam can be decomposed into left-handed and right-handed circularly polarized light after passing through the cascaded LCPG113, and then the first reflected light beam 204 will generate two circularly polarized diffracted lights with different propagation directions and opposite polarization rotation directions after being incident on the cascaded LCPG113, that is: a first left-handed circularly polarized beam 207 and a first right-handed circularly polarized beam 206; similarly, second reflected beam 205, after being incident on cascaded LCPG113, will produce two circularly polarized diffracted lights with different directions of propagation and opposite polarizations, namely: second left-handed circular polarized light beam 208 and second right-handed circular polarized light beam 209, wherein first left-handed circular polarized light beam 207 and second right-handed circular polarized light beam 209 travel in the same direction (return in the opposite direction of the incident light) and have opposite polarization directions, and first right-handed circular polarized light beam 206 and second left-handed circular polarized light beam 208 travel in different directions and also travel in different directions than first left-handed circular polarized light beam 207 and second right-handed circular polarized light beam 209.
According to the measurement principle of the system, when the emitters are configured to emit light beams by the light source array, the light beams emitted by each light source are incident on the cascaded LCPG at different angles after passing through the light beam shaping assembly to generate a first diffracted light beam and a second diffracted light beam which are respectively projected to the first area and the second area, and the first reflected light beam and the second reflected light beam reflected by the two areas respectively generate two circularly polarized light beams after passing through the cascaded LCPG. The first left-handed circularly polarized light beam formed after being reflected by the first area is transmitted along the opposite direction of the incident light beam, and the first right-handed circularly polarized light beam is transmitted by other light paths; the second right-handed circularly polarized light beam formed after the reflection of the second area is transmitted along the opposite direction of the incident light path, and the second left-handed circularly polarized light beam is transmitted by other light paths. The imaging area of the first left-handed circularly polarized light beam and the imaging area of the second right-handed circularly polarized light beam which are incident on the pixel unit are not changed by changing the number of the opening layers of the cascade LCPG; and the imaging area of the first right-handed polarized light beam and the second left-handed polarized light beam incident on the pixel unit is shifted.
Fig. 3a and 3b are schematic diagrams of a pixel unit in an embodiment of the invention. The polarization selection component selects two circularly polarized light beams to ensure that only one circularly polarized light beam is transmitted at the same time and forms a polarized light beam to be incident on the pixel unit, wherein the polarized light beam can be a circularly polarized light beam or a linearly polarized light beam. For example: only left-handed circularly polarized light or right-handed circularly polarized light is enabled to form linearly polarized light beams to be incident on the pixel unit after passing through the polarization selection assembly at the same time; or, the two circularly polarized light beams are ensured to form polarized light beams with different polarization directions respectively through the polarization selection component and to be respectively incident on different pixel units at the same time.
In one embodiment, when the emitter emits a spot beam toward the object to be measured, the optical elements in the collector direct the spot beam to the corresponding pixels to form an imaging spot, and generally, the size of a single spot can be set to correspond to a plurality of pixels, so as to ensure that as many reflected light signals as possible are received. In the present invention, it is assumed that each spot corresponds to a pixel unit, i.e. the position of each reflected spot beam imaged onto the pixel unit corresponds to the position of the pixel.
In one embodiment, it is ensured that only left-circularly polarized light beams pass through the polarization selection component and are incident on the pixel unit, and at this time, a first overlapping region 301 appears in a corresponding imaging region (indicated by a hollow circle in fig. 3 a) of the first left-circularly polarized light beam on the pixel unit and a corresponding imaging region (indicated by a shaded circle in fig. 3 b) of the second left-circularly polarized light beam on the pixel unit; similarly, it is ensured that only the right-handed circularly polarized light beam passes through the polarization selection component and is incident on the pixel unit, and at this time, the first right-handed circularly polarized light beam and the second right-handed circularly polarized light beam correspondingly form a second overlapping region (not shown) on the pixel unit. In one embodiment, the polarization selection component is configured to ensure that two circularly polarized light beams are transmitted at the same time to form different polarized light beams to be respectively incident on different areas of the pixel unit, and the first overlapping area and the second overlapping area are formed at the same time. The following description will take the first overlapping area as an example, and the second overlapping area can be derived similarly, which is not described herein. The present invention will be specifically described below by taking a left-handed circularly polarized beam as an example.
As shown in fig. 3b, the pixel unit is a pixel array formed by a plurality of pixels 305, the first left-handed circularly polarized light beam and the second left-handed circularly polarized light beam pass through the polarization selection component to form a first polarized light beam and a second polarized light beam, and the first polarized light beam and the second polarized light beam are incident on the pixels in the pixel unit to form an overlapping region. There are three overlap cases at the first overlap region 301: in the first overlapping mode, the first polarized light beam and the second polarized light beam are incident on different pixel units to form non-coincident imaging light spots 302, each polarized light beam is respectively incident on different pixel units, and the control and processing circuit calculates the flight time according to the echo signals collected by the pixel units; in a second overlapping mode, the first polarized light beam and the second polarized light beam are incident on the same pixel unit to form a non-coincident imaging light spot 303, and each pixel 305 in the overlapping region receives both the first polarized light beam and the second polarized light beam, that is, two echo signals are detected and a test region corresponding to the echo signal cannot be distinguished; in the third overlapping mode, the first polarized light beam and the second polarized light beam are incident on the same pixel unit to form the overlapped imaging spot 304, and at this time, two echo signals are received on each pixel 305 of the overlapping area, so that the corresponding detection area cannot be distinguished.
In the embodiment of the present invention, the emitter and/or the collector are configured to enable a part of pixels on the pixel unit to receive the reflected light beam, so that the first reflected light beam and the second reflected light beam form a circularly polarized light beam after being diffracted by the cascaded LCPG, and a polarized light beam formed after each circularly polarized light beam passes through the polarization selection component is incident on one pixel in the pixel unit, that is: and the position of each polarized light beam formed after each circularly polarized light beam passes through the polarization selection assembly and is incident on the pixel unit in the overlapping area corresponds to each pixel in the pixel unit one by one. The control and processing circuit calculates the flight time between the emission and the reflection of the light beam to be collected, and further calculates the distance of the target.
Fig. 4 is a schematic diagram of the reflected light beam of the first embodiment of the present invention being imaged on the pixel unit. According to the grating equation of the single-layer LCPG and experimental research, the area size of the overlapping region is mainly related to four parameters of the system, which are respectively: the design parameters of the cascade LCPG, the area of a light source incident on the cascade LCPG, the angle of the light source emission beam incident on the cascade LCPG and the focal length of the imaging lens unit. By adjusting the parameters of the system, the first polarized light beam can be incident on the pixel unit to form a first imaging area 401, the second polarized light beam can be incident on the pixel unit to form a second imaging area 402, at this time, the first overlapping area disappears, only one polarized light beam is received on each pixel, the measurement error caused by the overlapping of light spots is effectively solved, and similarly, the second overlapping area also disappears.
It will be appreciated that in this embodiment the light source is an array of light sources comprising a plurality of light sources, optically shaped by a beam shaping assembly, and then emitting a spot pattern beam, a flood beam, a line beam or an array of line beams into space.
In one embodiment, the design parameters of the cascaded LCPG are adjusted, including adjusting the pitch of the single-layer LCPG, the gate line direction of each layer of LCPG, whether a 1/2 wave plate is arranged, and the like, for example, when a beam is perpendicularly incident on the cascaded LCPG, the design parameters of the cascaded LCPG are adjusted, so that the diffraction angle of the beam is gradually increased, and the area of the overlapping region is gradually reduced. The overlapping area of the first polarized light beam and the second polarized light beam incident on the pixel unit can be reduced and disappeared by reasonably adjusting the design parameters of the cascade LCPG.
In one embodiment, the area of the light source incident on the cascaded LCPGs is adjusted so that the smaller the area, the smaller the area of the overlap region, and the overlap region disappears by designing the beam shaping component so that the area of the light source incident on the LCPGs is sufficiently small.
In one embodiment, the angle at which the light source emission beams are incident on the cascaded LCPGs is adjusted, and the larger the angle, the smaller the area of the overlapping region. For example, the overlapping area may be eliminated by adjusting the design parameters of the beam shaping component such that the angle at which the light source passes through the shaping component and is incident on the cascaded LCPGs is increased.
In one embodiment, the focal length of the imaging lens unit is adjusted, and the larger the focal length, the smaller the area of the overlapping region. The focal length of the imaging lens unit is increased by configuring it so that the overlapping area disappears.
It can be understood that the above system parameter adjustment can be adjusted individually to implement the disappearance of the overlapping area, or some or all of the system parameters can be adjusted by reasonable design to cause the disappearance of the overlapping area, and the specific design scheme is not limited herein.
Fig. 5 is a schematic diagram of a reflected light beam imaging spot according to a second embodiment of the invention. Due to the fact that the first polarized light beam and the second polarized light beam are incident on the same pixel to form overlapping, the pixel unit cannot identify whether the received light signal comes from the first area or the second area. In the embodiment shown in fig. 5, by reasonably designing the arrangement of the light source arrays, even if there is an overlapping region, it can be ensured that the incident light beams are incident on different pixel units in a non-overlapping manner to form the overlapping region, and only one polarized light beam is received at each pixel, and at this time, the received reflected light beams can be calculated to obtain the flight time.
The specific design mode is as follows: the method comprises the steps that a first light source is used as a sample point, the position of the sample point is assumed to be located at the center of a light source array, light emitted by the light source is controlled to be incident on a cascade liquid crystal polarization grating at a certain angle, the number of opened layers of the cascade liquid crystal polarization grating is adjusted to obtain a group of imaging light spots, and the arrangement mode of the light source array is designed according to the distribution relation of the imaging light spots on pixel units; wherein, every time a new light source array is formed by adding one light source, the design process is repeated by taking the added light source as a sample point.
On one hand, as the angle of different light beams incident on the cascade LCPG is increased, the distance of formed imaging light spots is gradually increased; on the other hand, as the number of the opening layers of the cascaded LCPG is gradually increased, the distance between imaging light spots formed on the pixel units by the same light beam is also gradually increased. According to the relation, firstly, light beams emitted by the first light source are controlled to be incident on the cascade LCPG at a certain angle, the number of layers for starting the cascade LCPG is controlled to be gradually increased, and first and second polarized light beams formed after first and second left-handed circularly polarized light beams reflected from a target area pass through the polarization selection component when each layer of LCPG is started form a first imaging light spot and a second imaging light spot on the pixel unit. And the first imaging light spots obtained by adjusting the number of the opening layers each time are all located at the same position of the pixel unit, namely the first imaging light spots are formed by the polarized light beams incident on the pixel unit along the direction opposite to the propagation direction of the incident light beams, and the second imaging light spots are formed by the polarized light beams incident on the pixel unit along the direction different from the propagation direction of the incident light beams and are not overlapped with the first imaging light spots, so that a group of imaging light spots are obtained.
According to the working principle of the distance measuring system, the first imaging light spot is formed by enabling the light beam reflected back from the first area to be incident on the pixel unit, the second imaging light spot is formed by enabling the light beam reflected back from the second area to be incident on the pixel unit, in order to ensure that the light spot imaged on the pixel unit by the light beam reflected back from the first area is not overlapped with the light spot imaged by the light beam returned back from the second area, the arrangement mode of the obtained group of imaging light spots is used as a template, and the arrangement of the light source array is designed according to the template.
Specifically, a first light source is used as a sample point and is configured at a central original point of a preset light source array, a first imaging light spot formed by the first light source on a pixel unit correspondingly is used as a reference light spot, an intermediate position between a second imaging light spot with the minimum distance to the reference light spot on the pixel unit is determined according to system geometric parameters, the number of opening layers of cascaded LCPG and diffraction characteristics, the intermediate position is assumed to be the first imaging light spot formed by the second light source by the incident of a reflected light beam on the pixel unit after the second light source emitting light beam is projected on a first area, and the corresponding position of the second light source on the light source array is determined according to a light beam propagation path.
Then, the second light source is used as a new sample point, the light beam emitted by the second light source is controlled to be incident on the cascade liquid crystal polarization grating at a certain angle, and the number of layers of the cascade liquid crystal polarization grating is adjusted to obtain a group of imaging light spots again. And determining that the middle position between the first imaging light spot formed by the second light source and the second imaging light spot (including the second imaging light spots generated by the first light source and the second light source) with the minimum distance from the reference light spot is set as the first imaging light spot formed by the third light source, and confirming the corresponding position of the third light source on the light source array according to the light beam propagation path.
If the distance between the newly set first imaging light spot and the determined first imaging light spot (including the first imaging light spot formed by the first light source and the second light source) is found to be less than one pixel unit in the current setting, the intermediate position of the second imaging light spot with the second smallest distance from the reference light spot is selected and set as the first imaging light spot of the third light source. And if the distance between the newly set first imaging light spot and the determined first imaging light spot is found to be less than one pixel unit again, selecting the intermediate position of a second imaging light spot with the third smallest distance from the reference light spot as the first imaging light spot of the third light source. It can be understood that, in the setting process of the first imaging light spot corresponding to the third light source, the new first imaging light spot needs to be adjusted continuously by adjusting the selection of the second imaging light spot until the distance between the newly set first imaging light spot and the determined first imaging light spot is greater than one pixel unit, and the position of the third light source in the light source array is determined according to the position of the first imaging light spot.
In this embodiment, the method further includes a fourth light source, a fifth light source, and the like, and each time a light source is added, the light source is used as a sample point, a first imaging light spot formed on a pixel unit by the light source is used as a reference light spot, the above-described determination process of the light source position is repeated, and the process is repeated until an optimally designed light source array is formed.
After the arrangement mode of the light source array is redesigned, the emitted light beam is shaped by the light beam shaping assembly, and then, for example, a spot pattern light beam, a linear light beam or a linear light beam array can be emitted to a target area, after the two reflected light beams are subjected to the diffraction effect of the cascaded LCPG, the first polarized light beam forms a first imaging light spot 501 on the pixel unit, the second polarized light beam forms a second imaging light spot 502 on the pixel unit, and at the overlapping area, the first imaging light spot and the second imaging light spot are respectively positioned on different pixel units in a non-overlapping mode.
Fig. 6 is a schematic diagram showing an image formed by the reflected light beam on the pixel unit according to the third embodiment of the present invention. According to the principle of distance measurement, when polarized light beams are incident on the same pixel unit to form non-coincident imaging light spots, the minimum distance d is formed between the imaging light spots of the first polarized light beam and the second polarized light beam which are incident on the pixel unit, on the other hand, the light spot distribution formed by the first polarized light beam which is incident on the pixel unit is in a corresponding relation with the light source distribution, the distance between each light spot and the size of each light spot can be calculated, therefore, a mask can be designed according to the parameters, and only one polarized light beam can be incident on the pixel unit when the two polarized light beams are incident on the same pixel unit. It will be appreciated that in embodiments of the invention the light source is configured as an array of light sources comprising a plurality of light sources emitting a beam of light through a shaping assembly and towards a target area a speckle pattern beam.
The mask is arranged at the position where the polarized light beam transmitted along the incident light path in the opposite direction is incident on the pixel unit. For example, in the embodiment of the invention, the position where the first polarized light is incident on the pixel unit is arranged, the opening is arranged at the imaging position corresponding to the incident light beam, and the diameter of the opening is smaller than the minimum distance d, so that only the first polarized light beam is incident on the pixel array at the overlapping area to form the imaging spot 601.
It will be appreciated that in practice, the recipe for setting the reticle may be combined with adjusting system parameters and redesigning the light source, and is not limited to distinguishing the echo signals at the overlap region in a single recipe.
On the other hand, the invention also provides a method for analyzing the areas corresponding to the two echo signals received by the pixels at the overlapping area based on the flight time calculated after the echo signals are received.
Fig. 7 is a schematic structural diagram of a receiver according to a fourth embodiment of the present invention, in which a first reflected light beam reflected by a first region and a second reflected light beam reflected by a second region are irradiated onto the cascade LCPG113 and then diffracted to generate four polarized light beams, which are a first left-handed circularly polarized light beam, a first right-handed circularly polarized light beam, a second left-handed circularly polarized light beam, and a second right-handed circularly polarized light beam. The polarization selection component 123 selects the two polarized light beams to ensure that the two polarized light beams are respectively incident on different pixel units at the same time. The first left-handed circularly polarized light beam and the second left-handed circularly polarized light beam form different first polarized light beams and second polarized light beams after passing through the polarization selection component 123, and the first polarized light beams and the second polarized light beams are incident to the first pixel unit 706 through the first imaging lens unit 704; the first right-handed circularly polarized light beam and the second right-handed circularly polarized light beam form different third and fourth polarized light beams after passing through the polarization selection component 123, and enter the second pixel unit 707 through the second imaging lens unit 705. The first imaging lens unit 704 and the second imaging lens unit 705 have different focal lengths. In one embodiment, the first pixel unit and the second pixel unit may be two different imaging regions on one pixel unit.
In one embodiment, the polarization selection component 123 may include a 1/4 wave plate 701, a Polarization Beam Splitter (PBS) 702, and a mirror 703, wherein the 1/4 wave plate 701 receives the first and second left-handed polarized light beams and the first and second right-handed polarized light beams reflected by the target and emits the first, second, third, and fourth linearly polarized light beams, and the polarization directions of the first and second linearly polarized light beams and the third and fourth linearly polarized light beams are perpendicular to each other. Then, after the first, second, third, and fourth polarized light beams pass through the PBS702, two of the polarized light beams are transmitted and the other two polarized light beams are reflected; further, the transmitted first and second linearly polarized light beams are incident on the first pixel unit 706 through the first imaging lens 704 and collected, the reflected linearly polarized light beams are incident on the second pixel unit 707 through the second imaging lens 705 after passing through the reflecting mirror 703 and collected, and the reflecting mirror 703 may also be disposed on the transmission light path of the PBS 702. The left-handed circularly polarized light beams and the right-handed circularly polarized light beams are imaged on different pixel units simultaneously through reasonable arrangement of the PBS702 and the reflecting mirror 703, so that synchronous measurement is realized.
In one embodiment, the polarization selection component comprises a monolithic LCPG, and when the left circularly polarized light beam and the right circularly polarized light beam reflected by the target are incident on the monolithic LCPG, the two circularly polarized light beams are separated in space after being diffracted by the LCPG, and therefore, the two circularly polarized light beams are respectively incident on different pixel units, so that synchronous measurement can be realized. In some embodiments, the polarization-selection component may also include cascaded LCPGs.
In one embodiment, the polarization selection component includes a super surface (metasface) polarization grating, so that left-circularly polarized light and right-circularly polarized light beams reflected by the target are incident on the metasface polarization grating and then are respectively incident on different pixel units, thereby realizing synchronous measurement.
Fig. 8 is a schematic diagram of an imaging spot of a reflected light beam according to a fourth embodiment of the invention. On the first pixel unit 706, the first polarized light beam reflected by the first area is incident on the pixel unit to form a first imaging area 801, the second polarized light beam reflected by the second area forms a second imaging area 802, and the two imaging areas are partially overlapped to form a first overlapping area. On the second pixel unit 707, the third polarized light beam reflected by the first region forms a third imaging region 803, the fourth polarized light beam reflected by the second region forms a fourth imaging region 804, and the two regions partially overlap to form a second overlapping region. Wherein the areas of the first overlapping area and the second overlapping area are not equal. The positions of the first polarized light beam and the third polarized light beam incident on the pixel units have a one-to-one correspondence relationship, and the flight times obtained by collecting the polarized light beams on the corresponding pixel units and calculating are equal; the positions of the second polarized light beam and the fourth polarized light beam incident on the pixel units have a one-to-one correspondence relationship, and the flight times obtained by calculating the polarized light beams collected on the corresponding pixel units are equal.
In the non-overlapping area, each pixel unit receives an echo signal, and the echo signal is processed by a control and processing circuit to calculate first flight time or second flight time; in the overlapping area, each pixel unit receives two echo signals, the first flight time and the second flight time are obtained through calculation by the control and processing circuit, and the area from which the echo signals come cannot be determined, so that the control and processing circuit cannot directly calculate the distance information of the first area and the second area according to the reflected light beams acquired by the pixel units. Therefore, the measurement regions corresponding to the two flight times obtained at the overlapping region can be distinguished according to the flight time calculated by receiving the echo signals at the non-overlapping region.
The specific signal analysis process is as follows: taking a pixel point corresponding to an imaging light spot 805 on a non-overlapping area on the first imaging area 801 as a sample point, the light spot 805 is projected onto a pixel unit from a reflected light beam at a point a on the first area, and assuming that coordinates of the light spot imaged on the pixel unit are (m, n), the light spot receives only one echo signal on the corresponding pixel unit, and the first flight time t0 is obtained through calculation. Meanwhile, another polarized light beam is reflected at the point a and projected to the second pixel unit to form an imaging light spot 806 in the third imaging area (the positions of the light spots formed by the two polarized light beams reflected at the same point on the pixel unit in the two imaging areas are the same), assuming that the coordinates of the light spot imaged on the pixel unit are (p, q), since the light spot 806 is located at the overlapping area, an echo signal reflected from the point B on the second area is also received on the corresponding pixel unit, and two flight times t0 and t1 are obtained by processing and calculating the echo signal, so that the flight time corresponding to the point B is t 1.
Further, another polarized light beam is imaged on the first pixel unit at the point B to form an imaging light spot 807 on the second imaging area, and assuming that coordinates of the light spot imaged on the pixel unit are (u, v), since the light spot 807 is located at the overlapping area, an echo signal reflected from the point C on the first area is also received on the corresponding pixel unit, and the echo signal is processed and calculated to obtain two flight times t1 and t2, thereby obtaining the flight time corresponding to the point C as t 2.
Next, a polarized light beam is reflected from the point C on the first area and imaged on the second pixel unit to form an imaging light spot 808 on the third imaging area, and assuming that coordinates of the light spot imaged on the pixel unit are (w, z), since the light spot 807 is located at the overlapping area, an echo signal reflected from the point D on the second area is also received on the corresponding pixel unit, and the echo signal is processed and calculated to obtain two flight times t2 and t3, so that the flight time corresponding to the point D is t 3.
By analogy, the measurement region corresponding to the echo signal acquired by each pixel unit at the overlapping region can be determined. It can be understood that the flight time obtained according to the nth column of pixels in the first imaging region is assigned to the pixels at the same position in the third imaging region, the flight time corresponding to the imaging light spot in the overlapping region in the qth column in the fourth imaging region is further solved, the flight time of all the pixels in the qth column is assigned to the vth column in the second imaging region, the flight time corresponding to the imaging light spot in the overlapping region in the vth column is solved, and the flight time corresponding to the imaging light spot in the overlapping region in the vth column is obtained through the cyclic calculation process, so that the flight time calculated by each pixel unit corresponds to the first region or the second region. Controlling and processing circuitry to calculate a distance of the first region from a first time of flight corresponding to a pixel cell at the first or third imaging region; and calculating the distance of the second area according to the second flight time corresponding to the pixel unit at the second imaging area or the fourth imaging area.
It is to be understood that the foregoing is a more detailed description of the invention, and that specific embodiments are not to be considered as limiting the invention. It will be apparent to those skilled in the art that various substitutions and modifications can be made to the described embodiments without departing from the spirit of the invention, and these substitutions and modifications should be considered to fall within the scope of the invention. In the description herein, references to the description of the term "one embodiment," "some embodiments," "preferred embodiments," "an example," "a specific example," or "some examples" or the like are intended to mean that a particular feature, structure, material, or characteristic described in connection with the embodiment or example is included in at least one embodiment or example of the invention.
In this specification, the schematic representations of the terms used above are not necessarily intended to refer to the same embodiment or example. Furthermore, the particular features, structures, materials, or characteristics described may be combined in any suitable manner in any one or more embodiments or examples. Furthermore, various embodiments or examples and features of different embodiments or examples described in this specification can be combined and combined by one skilled in the art without contradiction. Although embodiments of the present invention and their advantages have been described in detail, it should be understood that various changes, substitutions and alterations can be made herein without departing from the scope of the invention as defined by the appended claims.
Moreover, the scope of the present application is not intended to be limited to the particular embodiments of the process, machine, manufacture, composition of matter, means, methods and steps described in the specification. One of ordinary skill in the art will readily appreciate that the above-disclosed, presently existing or later to be developed, processes, machines, manufacture, compositions of matter, means, methods, or steps, that perform substantially the same function or achieve substantially the same result as the corresponding embodiments described herein may be utilized. Accordingly, the appended claims are intended to include within their scope such processes, machines, manufacture, compositions of matter, means, methods, or steps.

Claims (10)

1. An off-axis scanning distance measuring system, comprising: comprises a transmitter, a collector and a control and processing circuit; wherein the content of the first and second substances,
the emitter comprises a light source for emitting a light beam, a light beam shaping component for shaping the light beam and a first cascade liquid crystal polarization grating; the first cascade liquid crystal polarization grating is used for diffracting the shaped light beam to generate a first diffracted light beam and a second diffracted light beam with opposite polarization rotation directions, the first diffracted light beam and the second diffracted light beam irradiate a target to be detected, and a first reflected light beam and a second reflected light beam are obtained through reflection;
the collector comprises a pixel unit, an imaging lens unit, a polarization selection component and a second cascade liquid crystal polarization grating; the second cascade liquid crystal polarization grating is used for receiving and diffracting at least part of the first reflected light beam and at least part of the second reflected light beam reflected by the target so as to respectively form two beams of circularly polarized light beams with opposite polarization directions and different propagation directions; the circularly polarized light beams with the same rotation direction of the first reflected light beam and the second reflected light beam form an overlapping area on the pixel unit after passing through the polarization selection component and the imaging lens unit;
the control and processing circuit is respectively connected with the emitter and the collector and is used for calculating the flight time between the emission and the collection of the light beam and calculating the distance of the target to be measured according to the flight time;
the emitter and/or the collector are configured to enable the position of each polarized light beam formed after each circularly polarized light beam passes through the polarization selection component, which is incident on the pixel units in the overlapping area, to correspond to each pixel in the pixel units in a one-to-one mode.
2. An off-axis scanning distance measuring system according to claim 1, characterized in that: the first diffracted light beam irradiates a first area on a target to be detected and reflects the first reflected light beam; the second diffracted light beam irradiates a second area on the target to be detected and reflects the second reflected light beam; the first reflected light beam forms a first left-handed circularly polarized light beam and a first right-handed circularly polarized light beam which have different propagation directions after passing through the cascade liquid crystal polarization grating; and the second reflected light beam passes through the cascade liquid crystal polarization grating to form a second left-handed circularly polarized light beam and a second right-handed circularly polarized light beam with different propagation directions.
3. An off-axis scanning distance measuring system according to claim 1, characterized in that: the cascade liquid crystal polarization grating comprises a plurality of layers of liquid crystal polarization gratings, and each layer of liquid crystal polarization grating is provided with a grating pitch and a grating line direction.
4. An off-axis scanning distance measuring system according to claim 1, characterized in that: and adjusting parameters for configuring the off-axis scanning distance measuring system to reduce the area of the overlapping region to disappear.
5. An off-axis scanning distance measuring system according to claim 1, characterized in that: the light source is an array light source, wherein the arrangement mode of the light source array is configured to enable the polarized light beams to be incident to different pixel units in a non-coincident mode to form the overlapping area.
6. An off-axis scanning distance measuring system according to any of claims 1-5, wherein: the mask is configured to enable only one polarized light beam to be incident on the same pixel unit when the polarized light beams are incident on the same pixel unit.
7. An off-axis scanning distance measuring system according to claim 4, characterized in that: the parameters comprise one or more of design parameters of the cascade liquid crystal polarization grating, the area of a light source incident on the cascade liquid crystal polarization grating, the angle of a light source emission beam incident on the cascade liquid crystal polarization grating and the focal length of the imaging lens unit.
8. An off-axis scanning distance measuring system according to claim 5, characterized in that: a light source is used as a sample point, a light beam emitted by the light source is controlled to be incident on the cascade liquid crystal polarization grating at a certain angle, the number of opened layers of the cascade liquid crystal polarization grating is adjusted to obtain a group of imaging light spots, and the arrangement mode of the light source array is designed according to the distribution relation of the imaging light spots on the pixel units; and repeating the design process by taking the added light sources as sample points.
9. An off-axis scanning distance measuring system according to claim 6, wherein: designing the mask plate according to the space between light spots formed by the polarized light beams incident on the pixel units and the sizes of the light spots; and arranging the mask at the position where the polarized light beam transmitted along the opposite direction of the incident light path is incident on the pixel unit.
10. An off-axis scanning distance measuring system according to claim 7, wherein: the design parameters of the cascade liquid crystal polarization grating comprise the grating pitch of a single-layer liquid crystal polarization grating and the grating line direction of each layer of liquid crystal polarization grating.
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