The present invention relates to a laser radar for detecting an object by using laser light.
In recent years, a laser radar has been used for the security purpose of detecting intrusion into a building, etc. Generally, the laser radar scans a target region with laser light, and detects the presence/absence of an object at each scanning position on the basis of reflected light at each scanning position. In addition, the laser radar detects the distance to the object at each scanning position on the basis of the time taken from the irradiation timing of the laser light to the reception timing of the reflected light at each scanning position.
Japanese Patent No. 6069281 describes a detection device including a stationary pedestal and a scanning part which rotates about a rotation axis with respect to the pedestal, and states that a plurality of detection units are housed in the scanning part in the circumferential direction about the rotation axis and rotate together with the scanning part, and an object is detected, for example, by using laser light.
In the above-described detection device, a range in the circumferential direction about the rotation axis is scanned by the detection units rotating about the rotation axis. However, there is a limit to expanding the laser light with a single lens, so that it is difficult to expand the scanning range in a direction parallel to the rotation axis.
A laser radar according to a first aspect of the present invention includes: a base member; a drive part configured to rotate the base member about a rotation axis; and a plurality of optical units arranged on the base member at a predetermined interval in a circumferential direction about the rotation axis and each configured to project laser light in a direction away from the rotation axis. Projection directions of the laser lights from the plurality of optical units are different from each other in a direction parallel to the rotation axis.
With the laser radar according to this aspect, when the base member rotates about the rotation axis, a range in the circumferential direction centered on the rotation axis is scanned with the laser light emitted from each optical unit. At this time, since the projection directions of the laser lights from the respective optical units are different from each other in the direction parallel to the rotation axis, the ranges scanned with the respective laser lights are shifted from each other in the direction parallel to the rotation axis. Therefore, the entire range scanned with these laser lights is a wide range obtained by integrating the scanning ranges of the respective laser lights shifted from each other in the direction parallel to the rotation axis. Therefore, the scanning range in the direction parallel to the rotation axis can be effectively expanded.
A laser radar according to a second aspect of the present invention includes: a base member; a drive part configured to rotate the base member about a rotation axis; and a plurality of optical units arranged on the base member at a predetermined interval in a circumferential direction about the rotation axis and each configured to project laser light in a direction away from the rotation axis. Projection directions of the laser lights from the plurality of optical units are the same in a direction parallel to the rotation axis.
With the laser radar according to this aspect, the projection directions of the laser lights from the respective optical units are the same in the direction parallel to the rotation axis. Accordingly, the detection frequency for a range around the rotation axis can be increased, so that a high frame rate can be achieved without increasing the rotation speed.
It should be noted that the drawings are solely for description and do not limit the scope of the present invention by any degree.
Hereinafter, an embodiment of the present invention will be described with reference to the drawings. For convenience, in each drawing, X, Y, and Z axes that are orthogonal to each other are additionally shown. The Z-axis positive direction is the height direction of a laser radar 1.
As shown in
The base member 20 is installed on a drive shaft 13a of a motor 13 (see
The disk member 30 is a plate member having an outer shape that is a disk shape. In the disk member 30, six circular holes are formed at equal intervals (60° intervals) along the circumferential direction about the rotation axis R10. Each hole 31 penetrates the disk member 30 in the direction of the rotation axis R10 (Z-axis direction). The disk member 30 is installed on the upper surface of the base member 20 such that the six holes 31 are respectively positioned above the six installation surfaces 21 of the base member 20.
Each optical unit 40 includes a structure 41 and a mirror 42. The structure 41 includes two holding members 41a and 41b, a light blocking member 41c, and two substrates 41d and 41e. The holding members 41a and 41b and the light blocking member 41c hold each component of an optical system included in the structure 41. The holding member 41b is installed on an upper portion of the holding member 41a. The light blocking member 41c is held by the holding member 41a. The substrates 41d and 41e are installed on the upper surfaces of the holding members 41a and 41b, respectively. The structure 41 emits laser light in the downward direction (Z-axis negative direction), and receives laser light from the lower side. The optical system included in the structure 41 will be described later with reference to
As shown in
Subsequently, a substrate 50 is installed on the upper surfaces of the six optical units 40 as shown in
Then, in the state shown in
In detecting an object by the laser radar 1, laser light (projection light) is emitted from a laser light source 110 (see
The rotary part 60 shown in
The laser radar 1 determines whether or not an object exists in the scanning region, on the basis of whether or not the reflected light is received. In addition, the laser radar 1 measures the distance to the object existing in the scanning region, on the basis of the time difference (time of flight) between the timing when the projection light is projected to the scanning region and the timing when the reflected light is received from the scanning region. When the rotary part 60 rotates about the rotation axis R10, the laser radar 1 can detect objects that exist in substantially the entire range of 360 degrees around the laser radar 1.
As shown in
The support base 11 is made of, for example, a resin. The lower surface of the support base 11 is closed by the bottom plate 12 having a circular dish shape. A hole 11a is formed at the center of the upper surface of the support base 11 so as to penetrate the upper surface of the support base 11 in the Z-axis direction. The upper surface of the motor 13 is located around the hole 11a on the inner surface of the support base 11. The motor 13 includes the drive shaft 13a extending in the Z-axis positive direction, and rotates the drive shaft 13a about the rotation axis R10.
The non-contact power feeding part 211 is installed around the hole 11a on the outer surface of the support base 11 along the circumferential direction about the rotation axis R10. The non-contact power feeding part 211 is composed of a coil capable of supplying power to and being supplied with power from a non-contact power feeding part 171 described later. In addition, the non-contact communication part 212 is installed around the non-contact power feeding part 211 on the outer surface of the support base 11 along the circumferential direction about the rotation axis R10. The non-contact communication part 212 is composed of a substrate on which electrodes and the like capable of wireless communication with a non-contact communication part 172 described later are arranged.
A control part 201 and a power supply circuit 202 (see
A hole 22 is formed at the center of the base member 20 so as to penetrate the base member 20 in the Z-axis direction. By installing the drive shaft 13a of the motor 13 in the hole 22, the base member 20 is supported on the fixing part 10 so as to be rotatable about the rotation axis R10. The non-contact power feeding part 171 is installed around the hole 22 on the lower surface side of the base member 20 along the circumferential direction about the rotation axis R10. The non-contact power feeding part 171 is composed of a coil capable of supplying power to and being supplied with power from the non-contact power feeding part 211 of the fixing part 10. In addition, the non-contact communication part 172 is installed around the non-contact power feeding part 171 on the lower surface side of the base member 20 along the circumferential direction about the rotation axis R10. The non-contact communication part 172 is composed of a substrate on which electrodes and the like capable of wireless communication with the non-contact communication part 212 of the fixing part 10 are arranged.
As described with reference to
The structure 41 of each optical unit 40 includes the laser light source 110, the collimator lens 120, a condensing lens 130, a filter 140, and the photodetector 150 as components of the optical system.
Holes are formed in the holding members 41a and 41b and the light blocking member 41c so as to penetrate the holding members 41a and 41b and the light blocking member 41c in the Z-axis direction. The light blocking member 41c is a tubular member. The laser light source 110 is installed on the substrate 41d installed on the upper surface of the holding member 41a, and the emission end face of the laser light source 110 is positioned inside the hole formed in the light blocking member 41c. The collimator lens 120 is positioned inside the hole formed in the light blocking member 41c, and is installed on the side wall of this hole. The condensing lens 130 is held in the hole formed in the holding member 41a. The filter 140 is held in the hole formed in the holding member 41b. The photodetector 150 is installed on the substrate 41e installed on the upper surface of the holding member 41b.
A control part 101 and a power supply circuit 102 (see
Each laser light source 110 emits laser light (projection light) having a predetermined wavelength. The emission optical axis of the laser light source 110 is parallel to the Z-axis. The collimator lens 120 converges the projection light emitted from the laser light source 110. The collimator lens 120 is composed of, for example, an aspherical lens. The projection light converged by the collimator lens 120 is incident on the mirror 42. The projection light incident on the mirror 42 is reflected by the mirror 42 in a direction away from the rotation axis R10. Then, the projection light passes through the cover 70 and is projected to the scanning region.
If an object exists in the scanning region, the projection light projected to the scanning region is reflected by the object. The projection light (reflected light) reflected by the object passes through the cover 70 and is guided to the mirror 42. Then, the reflected light is reflected in the Z-axis positive direction by the mirror 42. The condensing lens 130 converges the reflected light reflected by the mirror 42.
Then, the reflected light is incident on the filter 140. The filter 140 is configured to allow light in the wavelength band of the projection light emitted from the laser light source 110 to pass therethrough and to block light in the other wavelength bands. The reflected light having passed through the filter 140 is guided to the photodetector 150. The photodetector 150 receives the reflected light and outputs a detection signal corresponding to the amount of the received light. The photodetector 150 is, for example, an avalanche photodiode.
As shown in
The reflected light from the scanning region is reflected in the Z-axis positive direction by the mirror 42 and is then incident on the condensing lens 130. An optical axis A1 of a projection optical system (the laser light source 110 and the collimator lens 120) for projecting the projection light and an optical axis A2 of a light-receiving optical system (the condensing lens 130) for receiving the reflected light are each parallel to the Z-axis direction and are separated from each other by a predetermined distance in the circumferential direction about the rotation axis R10.
Here, in the present embodiment, the optical axis A1 of the projection optical system is included in the effective diameter of the condensing lens 130, and thus an opening 131 through which the optical axis A1 of the projection optical system passes is formed in the condensing lens 130. The opening 131 is formed on the outer side with respect to the center of the condensing lens 130, and is a cutout penetrating the condensing lens 130 in the Z-axis direction. By providing the opening 131 in the condensing lens 130 as described above, the optical axis A1 of the projection optical system and the optical axis A2 of the light-receiving optical system can be made closer to each other, and the laser light emitted from the laser light source 110 can be incident on the mirror 42 almost without being incident on the condensing lens 130.
The light blocking member 41c shown in
In the present embodiment, the rotary part 60 is rotated clockwise about the rotation axis R10 when viewed in the Z-axis negative direction. Accordingly, each component of the optical unit 40 located on the X-axis positive side of the rotation axis R10 shown in
As shown in
As shown in
The six optical units 40 rotate about the rotation axis R10. At this time, the six optical units 40 project the projection light in directions away from the rotation axis R10 (radially as viewed in the Z-axis direction). While rotating at a predetermined speed, the six optical units 40 project the projection light to the scanning region, and receive the reflected light from the scanning region. Accordingly, object detection is performed over the entire circumference (360°) around the laser radar 1.
As described above, the installation angles of the six mirrors 42 are different from each other. Accordingly, the angles of six fluxes L1 to L6 of the projection light emitted from the six optical units 40, respectively, are also different from each other. In
The laser radar 1 includes the control part 101, the power supply circuit 102, a drive circuit 161, a processing circuit 162, the non-contact power feeding part 171, the non-contact communication part 172, the control part 201, the power supply circuit 202, the non-contact power feeding part 211, and the non-contact communication part 212 as components of circuitry. The control part 101, the power supply circuit 102, the drive circuit 161, the processing circuit 162, the non-contact power feeding part 171, and the non-contact communication part 172 are disposed in the rotary part 60. The control part 201, the power supply circuit 202, the non-contact power feeding part 211, and the non-contact communication part 212 are disposed in the fixing part 10.
The power supply circuit 202 is connected to an external power supply, and power is supplied from the external power supply to each component of the fixing part 10 via the power supply circuit 202. The power supplied to the non-contact power feeding part 211 is supplied to the non-contact power feeding part 171 in response to the rotation of the rotary part 60. The power supply circuit 102 is connected to the non-contact power feeding part 171, and the power is supplied from the non-contact power feeding part 171 to each component of the rotary part 60 via the power supply circuit 102.
The control parts 101 and 201 each include an arithmetic processing circuit and a memory, and are each composed of, for example, an FPGA or MPU. The control part 101 controls each component of the rotary part 60 according to a predetermined program stored in the memory thereof, and the control part 201 controls each component of the fixing part 10 according to a predetermined program stored in the memory thereof. The control part 101 and the control part 201 are communicably connected to each other via the non-contact communication parts 172 and 212.
The control part 201 is communicably connected to an external system. The external system is, for example, an intrusion detection system, a car, a robot, or the like. The control part 201 drives each component of the fixing part 10 in accordance with the control from the external system, and transmits a drive instruction to the control part 101 via the non-contact communication parts 212 and 172. The control part 101 drives each component of the rotary part 60 in accordance with the drive instruction from the control part 201, and transmits a detection signal to the control part 201 via the non-contact communication parts 172 and 212.
The drive circuit 161 and the processing circuit 162 are provided in each of the six optical units 40. The drive circuit 161 drives the laser light source 110 in accordance with the control from the control part 101. The processing circuit 162 performs processing such as amplification and noise removal on detection signals inputted from the sensors 151 of the photodetector 150, and outputs the resultant signals to the control part 101.
In the detection operation, while controlling the motor 13 to rotate the rotary part 60 at a predetermined rotation speed, the control part 201 controls the six drive circuits 161 to emit laser light (projection light) from each laser light source 110 at a predetermined rotation angle at a predetermined timing. Accordingly, the projection light is projected from the rotary part 60 to the scanning region, and the reflected light is received by the sensors 151 of the photodetector 150 of the rotary part 60. The control part 201 determines whether or not an object exists in the scanning region, on the basis of detection signals outputted from the sensors 151. In addition, the control part 201 measures the distance to the object existing in the scanning region, on the basis of the time difference (time of flight) between the timing when the projection light is projected and the timing when the reflected light is received from the scanning region.
According to the embodiment described above, the following effects are achieved.
As shown in
Each optical unit 40 includes the laser light source 110 and the mirror 42 which bends the optical axis of the laser light source 110. In addition, as shown in
By using the mirror 42 as an optical element that bends the optical axis of the laser light source 110 as described above, the attenuation of the projection light emitted from the structure 41 can be suppressed, and the power of the projection light projected to the scanning range can be ensured.
In the base member 20, the six installation surfaces 21 for installing the mirrors 42 are formed in the installation regions in which the six optical units 40 are installed, respectively. In addition, the inclination angle of each of the six installation surfaces 21 with respect to the plane (X-Y plane) perpendicular to the optical axis of the laser light source 110 is different for each installation region of the optical unit 40. Accordingly, by merely installing the mirror 42 on each installation surface 21, the mirror 42 can be installed at a desired inclination angle on the base member 20. Therefore, the projection direction of the projection light projected from each optical unit 40 can be easily adjusted.
The laser light source 110 is a surface-emitting laser light source having a light emission surface that is longer in one direction. In addition, each optical unit 40 includes the collimator lens 120 on which the laser light (projection light) emitted from the laser light source 110 is incident. Furthermore, the laser light source 110 is installed such that the longitudinal direction of the light emission surface of the laser light source 110 coincides with the direction (Z-axis direction) parallel to the rotation axis R10 when the projection light is projected. Accordingly, the projection light projected from the optical unit 40 can be smoothly expanded in the direction (Z-axis direction) parallel to the rotation axis R10.
The photodetector 150 includes the six sensors 151 separated from each other in a direction (X-axis direction) corresponding to the direction (Z-axis direction) parallel to the rotation axis R10. Accordingly, the reflected light from each position in the scanning region in the direction parallel to the rotation axis R10 can be received by each sensor 151. Therefore, the state at each position in the scanning region can be detected on the basis of an output signal from each sensor 151.
As shown in
As shown in
As shown in
<Modification>
In the configuration in which the six optical units 40 are arranged at equal intervals (60° intervals) along the circumferential direction about the rotation axis R10 as in the above embodiment, control in which the six optical units 40 are caused to simultaneously emit light at the timing when the six optical units 40 are respectively positioned at angle positions obtained when the entire circumference is equally divided, can be performed. For example, when the rotary part 60 is rotated at a constant angular velocity, control in which the six optical units 40 are caused to simultaneously emit light every time the rotary part 60 rotates by an angle (for example, 1°) by which the entire circumference is equally divided, is performed. Accordingly, at an angle position at which the projection light is projected in one optical unit 40, the projection light can be projected from the optical unit 40 following the one optical unit 40. That is, the projection position of the projection light in each optical unit 40 can be caused to coincide in the circumferential direction. Accordingly, the detection position of an object by each projection light can also be caused to coincide in the circumferential direction. As a result, when a distance image of the entire circumference of the scanning range is generated by integrating the measured distances at the respective detection positions, the distance image can be smoothly generated.
However, the control in which the six optical units 40 are caused to simultaneously emit light as described above has a problem that the instantaneous power consumption is high and the control becomes complicated. Therefore, it is preferable that the respective optical units 40 are caused to emit light at different timings.
Therefore, in the present modification, a configuration for causing the projection position of the projection light in each optical unit 40 to coincide in the circumferential direction while causing the respective optical units 40 to emit light at different timings, is used.
First, the fact that the emission positions (emission angles with respect to a reference angle position) in the circumferential direction of the six optical units 40 are shifted from each other when the six optical units 40 are caused to sequentially emit light at equally spaced timings while rotating the rotary part 60 at a constant angular velocity in the case where the six optical units 40 are arranged at equal intervals as in the above embodiment, will be described below with reference to
For convenience, the six optical units 40 are referred to as optical units U1, U2, U3, U4, U5, and U6. The optical units U1 to U6 are arranged at 60° intervals along the circumferential direction about the rotation axis R10. When viewed in the Z-axis negative direction, the position on the X-axis positive side of the rotation axis R10 is defined as 0° (reference angle position), an angle clockwise from 0° is defined as a positive angle, and an angle counterclockwise from 0° is defined as a negative angle. In addition, the six optical units U1 to U6 rotate clockwise at a constant angular velocity ω (deg/sec).
It is assumed that the optical unit U1 at the position of 0° at time T1 rotates to the position at an angle d (deg) at time T2, and the six optical units U1 to U6 are caused to sequentially emit light at equal time intervals during this period. The angle by which the six optical units U1 to U6 rotate while being caused to sequentially emit light as described above is referred to as a light emission angle interval d. In addition, the time required for the optical units U1 to U6 to rotate by the light emission angle interval d is referred to as a light emission time interval Ti. The light emission time interval Ti can be represented by d/ω.
After the optical unit U1 is caused to emit light at time T1, the optical units U2 to U6 are caused to sequentially emit light until the light emission time interval Ti elapses to reach time T2. Here, the light emission interval of each optical unit is referred to as an adjacent light emission time interval A. The adjacent light emission time interval A is obtained by dividing the light emission time interval Ti by the number of optical units (six in this example), and can be represented by Ti/6.
Next, the emission angles of the six optical units U1 to U6 when the laser lights (projection lights) are emitted from the six optical units U1 to U6 at the light emission timings as in
As shown in
The time from the time when the optical unit U1 emits light to the time when the optical unit U2 emits light is the adjacent light emission time interval A as shown in
Subsequently, the optical units U1 to U6 rotate by the angle α during the period from the time when the optical unit U2 emits light to the time when the adjacent light emission time interval A elapses. Therefore, as shown in
Similarly, as shown in
Subsequently, by advancing by the angle α from the state of
The light emission of the six optical units U1 to U6 (light emission in one frame) performed while the six optical units U1 to U6 rotate by the light emission angle interval d (while the light emission time interval Ti elapses) is repeated. When the six optical units U1 to U6 have rotated 360°, the emission positions (emission angles) of the six optical units U1 to U6 are shifted from each other in the horizontal direction (circumferential direction) as shown in
As described above, it can be seen that in the case where the six optical units U1 to U6 are arranged at equal intervals, when the six optical units U1 to U6 rotate about the rotation axis R10 at a constant angular velocity and are caused to emit light at equal time intervals (adjacent light emission time intervals A), the emission angles (light-reception angles) of the reflected lights received by the six optical units U1 to U6 are shifted from each other. If the emission angles are shifted from each other as described above, when a distance image is generated on the basis of the detection signals outputted from the six optical units U1 to U6, the generated image is distorted. Therefore, further processing for correcting this distortion is required.
In the present modification, the arrangement of the six optical units U1 to U6 is changed from the arrangement at equal intervals in order to reduce such shift of the emission angles in the six optical units U1 to U6.
In the present modification, the optical unit U1 is disposed at the position of 0°. The optical unit U2 is disposed so as to be spaced apart from the optical unit U1 by 60°+a in the negative rotation direction. Similarly, the optical unit U3 is disposed so as to be spaced apart from the optical unit U2 by 60°+α in the negative rotation direction. The optical unit U4 is disposed so as to be spaced apart from the optical unit U3 by 60°+α in the negative rotation direction. The optical unit U5 is disposed so as to be spaced apart from the optical unit U4 by 60°+α in the negative rotation direction. The optical unit U6 is disposed so as to be spaced apart from the optical unit U5 by 60°+α in the negative rotation direction. Accordingly, the interval between the optical unit U1 and the optical unit U6 is 60°−5α.
As shown in
During the period from the time when the optical unit U1 emits light to the time when the adjacent light emission time interval A elapses, the optical units U1 to U6 rotate by the angle α. Therefore, as shown in
Similarly, as shown in
Subsequently, by advancing by the angle α from the state of
The light emission of the six optical units U1 to U6 (light emission in one frame) performed while the six optical units U1 to U6 rotate by the light emission angle interval d (while the light emission time interval Ti elapses) is repeated. In the present modification, when the six optical units U1 to U6 have rotated 360°, the emission positions (emission angles) of the six optical units U1 to U6 coincide in the horizontal direction (circumferential direction) as shown in
As described above, in the present modification, the six optical units U1 to U6 project laser light at times different from each other. Then, the installation position of each optical unit with respect to the base member 20 is set to a position displaced from an equal angle position in the circumferential direction by a predetermined angle, such that each optical unit projects laser light at the equal angle position in the circumferential direction.
Specifically, in the case where the six optical units U1 to U6 rotate at the constant angular velocity ω about the rotation axis R10 and are caused to emit light at equal time intervals (adjacent light emission time intervals A), the optical units U1 to U6 are disposed as shown in
<Other Modifications>
The configuration of the laser radar 1 can be modified in various ways other than the configuration shown in the above embodiment.
For example, in the above embodiment, the photodetector 150 includes the six sensors 151 separated from each other in the direction (radial direction of a circle centered on the rotation axis R10) corresponding to the direction (Z-axis direction) parallel to the rotation axis R10, but the number of sensors 151 disposed in the photodetector 150 is not limited thereto. For example, two to five sensors may be provided in the photodetector 150, or seven or more sensors may be provided in the photodetector 150. As the number of sensors disposed in the photodetector 150 is increased, the resolution of object detection in the direction parallel to the rotation axis R10 can be increased.
The photodetector 150 does not necessarily have to include a plurality of sensors, and may include one sensor 152 which is long in the radial direction from the rotation axis R10.
As shown in
According to this modification, the reflected light from each scanning range is received by one sensor 152. Therefore, although the resolution of the photodetector 150 corresponding to the Z-axis direction of each scanning range is lower than that of the above embodiment, the configuration of the photodetector 150 can be simplified. In addition, in this modification as well, similar to the above embodiment, the width in the Z-axis direction of the entire scanning range can be widened.
In the above embodiment, each laser light source 110 is a surface-emitting laser light source having a light emission surface that is longer in one direction, but is not limited thereto, and may be an end face-emitting laser light source.
As shown in
In this modification as well, similar to the above embodiment, the width in the Z-axis direction of the entire scanning range can be widened. However, in this modification, as shown in
In the above embodiment, the projection light is directed to the scanning region by the mirror 42, but a spectroscopic element that splits the projection light in the direction parallel to the rotation axis R10 may be further disposed. In this case, for example, a diffraction grating is used as the spectroscopic element.
The optical unit 40 of this modification includes a diffraction grating 180 between the collimator lens 120 and the mirror 42 as compared with the above embodiment. The diffraction grating 180 is installed inside the hole formed in the light blocking member 41c. The diffraction grating 180 is, for example, a step-type diffraction grating, and the diffraction efficiency thereof is adjusted such that the amounts of a 0th-order diffracted light beam, a +1st-order diffracted light beam, and a −1st-order diffracted light beam are substantially equal to each other. The projection light incident on the diffraction grating 180 from the collimator lens 120 is split into a 0th-order diffracted light beam, a +1st-order diffracted light beam, and a −1st-order diffracted light beam in the radial direction about the rotation axis R10 (X-axis direction in
According to this configuration, the projection range of the projection light is expanded in the direction parallel to the rotation axis R10 as compared with the above embodiment. Therefore, in order to obtain the same scanning range as that of the above embodiment, the six optical units 40 do not necessarily have to be disposed, and by adjusting the diffraction angle of the diffraction grating 180, for example, only two optical units 40 may be disposed in the base member 20.
When the two optical units 40 installed in this modification are referred to as optical units U1 and U2, the inclination angle of the mirror 42 of the optical unit U1 and the inclination angle of the mirror 42 of the optical unit U2 are different from each other. Therefore, as shown in
In this modification, three fluxes of the projection light corresponding to the optical unit U1 are projected, and three fluxes of the projection light corresponding to the optical unit U2 are projected. Therefore, the scanning range based on one optical unit is about three times as wide as that of the above embodiment. Therefore, as shown in
In this modification, by disposing the diffraction grating 180 in each of the optical units U1 and U2, the laser light projected from each of the optical units U1 and U2 can be split in the direction (Z-axis direction) parallel to the rotation axis R10 as described above. Accordingly, the scanning range by one optical unit can be expanded in the direction of the rotation axis R10. Therefore, the number of optical units disposed in the base member 20 can be reduced as compared with the above embodiment, so that the device can be simplified and the cost can be reduced.
According to this modification, the resolution of the photodetector 150 corresponding to the Z-axis direction of each scanning range is the same as that of the above embodiment. In addition, similar to the above embodiment, the length in the Z-axis direction of the entire scanning range is increased.
However, in this modification, since the laser light emitted from each laser light source 110 is split by the diffraction grating 180, the amount of the projection light based on each diffracted light beam is smaller than the amount of the projection light based on one optical unit 40 of the above embodiment. Therefore, in order to increase the detection limit distance, it is necessary to increase the emission power of the laser light source 110 and increase the amount of the projection light based on each diffracted light beam.
In the modification shown in
In the modification shown in
In the modification shown in
In the above embodiment, the six optical units 40 are installed along the circumferential direction about the rotation axis R10, but the number of optical units 40 installed is not limited to six, and may be two to five, or may be seven or more.
In the above embodiment, a plurality of the optical units 40 are arranged at equal intervals (60° intervals) along the circumferential direction about the rotation axis R10, but do not necessarily have to be installed at equal intervals.
In the above embodiment, the motor 13 is used as a drive part that rotates the rotary part 60, but instead of the motor 13, a coil and a magnet may be disposed in the fixing part 10 and the rotary part 60, respectively, to rotate the rotary part 60 with respect to the fixing part 10. In addition, a gear may be provided on the outer peripheral surface of the rotary part 60 over the entire circumference, and a gear installed on a drive shaft of a motor installed in the fixing part 10 may be meshed with this gear, whereby the rotary part 60 may be rotated with respect to the fixing part 10.
In the above embodiment, the projection directions of the projection lights projected from the respective optical units 40 are set to directions different from each other, by installing the mirrors 42 of the respective optical units 40 at inclination angles different from each other, but the method for making the projection directions of the projection lights projected from the respective optical units 40 different from each other is not limited thereto.
For example, the mirror 42 may be omitted from each of the six optical units 40, and six structures 41 may be radially installed such that the inclination angles thereof with respect to a plane perpendicular to the rotation axis R10 are different from each other. Alternatively, in the above embodiment, the mirror 42 may be omitted, and instead, the installation surface 21 may be subjected to mirror finish such that the reflectance of the installation surface 21 is increased. Still alternatively, in the above embodiment, each optical unit 40 includes one mirror 42, but may include two or more mirrors. In this case, the angle, with respect to the Z-axis direction, of the projection light reflected by a plurality of mirrors and projected to the scanning region may be adjusted on the basis of the angle of one of the plurality of mirrors.
In the above embodiment, the mirror 42 is used to bend the optical axis of the projection light emitted from the structure 41, but the optical axis of the projection light may be bent by a transmission-type optical element such as a diffraction grating instead of the mirror 42.
It is also possible to apply the structure according to the present invention to a device that does not have a distance measurement function and has only a function to detect whether or not an object exists in the projection direction on the basis of a signal from the photodetector 150. In this case as well, the scanning range in the direction (Z-axis direction) parallel to the rotation axis R10 can be expanded.
The configuration of the optical system of each optical unit 40 is not limited to the configuration shown in the above embodiment. For example, the opening 131 may be omitted from the condensing lens 130, and the projection optical system and the light-receiving optical system may be separated from each other such that the optical axis A1 of the projection optical system does not extend through the condensing lens 130. Furthermore, the number of laser light sources 110 disposed in the optical unit 40 is not limited to one, and may be plural. In this case, projection light may be generated by integrating the laser light emitted from each laser light source 110 with a polarization beam splitter or the like. This configuration is suitable, for example, for use in the modification in
In the above embodiment, in order to expand the scanning range in the direction parallel to the rotation axis, the projection directions of the projection lights projected from the plurality of the optical units 40 are made different from each other in the direction (Z-axis direction) parallel to the rotation axis R10. However, for other purposes, the projection directions of the projection lights projected from the plurality of the optical units 40 may be set to be the same in the direction (Z-axis direction) parallel to the rotation axis R10.
In addition to the above, various modifications can be made as appropriate to the embodiments of the present invention, without departing from the scope of the technological idea defined by the claims.
Number | Date | Country | Kind |
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2019-137672 | Jul 2019 | JP | national |
This application is a continuation of International Application No. PCT/JP2020/021728 filed on Jun. 2, 2020, entitled “LASER RADAR”, which claims priority under 35 U.S.C. Section 119 of Japanese Patent Application No. 2019-137672 filed on Jul. 26, 2019, entitled “LASER RADAR”. The disclosure of the above applications is incorporated herein by reference.
Number | Date | Country | |
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Parent | PCT/JP2020/021728 | Jun 2020 | US |
Child | 17570795 | US |