JP4955508B2 - Ranging device, ranging method and program - Google Patents

Description

  The present invention relates to a distance measuring device and method for generating a distance image representing a three-dimensional shape of a subject, and a program for causing a computer to execute the distance measuring method.

  Using the TOF (Time Of Flight) distance measurement method, which measures the distance to the subject using light reflection, the distance from the imaging device to the subject is measured, and the three-dimensional shape of the subject is determined. A distance image to be expressed is generated (see Patent Document 1). Specifically, distance measurement using the TOF method irradiates a subject with intensity-modulated distance-measuring light and reflects light at four phases of 0, π / 2, π, and 3π / 2 in this modulation period. The light receiving signal corresponding to the amount of received light is obtained, and the phase delay (phase difference) between the distance measuring light and the reflected light is detected for each light receiving element of the image sensor provided in the photographing apparatus based on the light receiving signal. Thus, distance information is calculated, and a distance image representing the three-dimensional shape of the subject is generated using the distance information as the pixel value of each pixel.

Further, when the distance is measured by the TOF method, the first distance measuring light intensity-modulated in a sine wave, a triangular wave or a sawtooth wave whose intensity changes with time, and the intensity is modulated in a pulse shape with a constant intensity. A technique for improving the distance measurement accuracy using the second distance measuring light has also been proposed (see Patent Document 2). The method described in Patent Document 2 calculates distance information by dividing a first received light signal obtained by first ranging light by a second received light signal obtained by second ranging light. Is.
JP 2006-84429 A JP 2001-313958 A

  By the way, when using distance measuring light that has been intensity-modulated so that its intensity changes with time, it is possible to calculate a phase difference whose maximum value is the length of the modulation period. Although the distance can be obtained, the intensity of the reflected light decreases depending on the phase of modulation of the distance measuring light. For this reason, since the S / N of the received light signal obtained by the influence of external light is lowered, the accuracy of distance measurement is not so high. On the other hand, when distance measuring light whose intensity is modulated in a pulse form is used, the intensity of the reflected light is constant, so that the S / N is hardly lowered and the distance can be measured with high accuracy. However, when using pulsed light, it is only possible to calculate the phase difference that maximizes the period during which pulsed light is emitted, so the range over which distance measurement can be performed is narrow, and only a limited range is available. Cannot measure distance.

  Here, in the method described in Patent Document 2, the distance information is calculated by dividing the light reception signal obtained by the first distance measurement light by the light reception signal obtained by the second distance measurement light. The distance measurement is performed by the first light receiving signal by the first distance measuring light whose intensity is modulated so that the intensity changes with time. For this reason, with the method described in Patent Document 2, the accuracy of distance measurement is not so high.

  The present invention has been made in view of the above circumstances, and an object thereof is to enable accurate and high-speed distance measurement.

The distance measuring device according to the present invention includes a first distance measuring light modulated such that the intensity changes with time in a predetermined period, and a second distance light modulated in a pulse wave having a constant intensity in the predetermined period. Ranging light emitting means for switching the ranging light so that it can be switched;
An imaging means having a plurality of light receiving elements for outputting a light reception signal corresponding to the amount of received light;
A light receiving control means for controlling a light receiving period of the imaging means;
Distance information calculating means for calculating distance information representing a distance to a subject for each light receiving element based on the light receiving signal;
The first ranging light is emitted, a plurality of first received light signals are acquired in a plurality of light receiving periods having different phases in a modulation period of the first ranging light, and the first received light signals are Based on this, a phase difference between the first distance measuring light and the reflected light of the first distance measuring light is calculated for each light receiving element, and emission of the second distance measuring light is started based on the phase difference. A phase is changed so as to be different from the light emission start phase of the first distance measuring light, the second distance measuring light is emitted, and a plurality of signals corresponding to the phase difference in the modulation period of the second distance measuring light are emitted. A plurality of second light reception signals are acquired during the light reception period, and the distance measurement light emission is performed so as to select a second light reception signal used for calculating the distance information based on the plurality of first light reception signals. And a control means for controlling the imaging means, the light reception control means, and the distance information calculation means. It is an feature.

  “Intensity modulation so that the intensity changes with time” means that the first distance-measuring light is modulated so that the intensity continuously changes with the passage of time. Specifically, the intensity can be modulated such that the intensity changes with time by modulating the intensity in a sine wave shape, a triangular wave shape, or a sawtooth wave shape.

  Here, when the first distance measuring light modulated so that the intensity varies with time can be measured by a relatively long range, the intensity of the reflected light depends on the phase of the modulation. Get smaller. For this reason, since the S / N of the received light signal obtained by the influence of external light is lowered, the accuracy of distance measurement is not so high. On the other hand, when using the second ranging light whose intensity is modulated in a pulse shape with a constant intensity, the intensity of the reflected light is constant, so that the S / N is hardly lowered and the ranging can be performed with high accuracy. . However, since the range in which distance measurement can be performed is limited by the pulse width, distance measurement can be performed only in a limited range.

  According to the present invention, based on the plurality of first light receiving signals obtained from the reflected light of the first distance measuring light, among the plurality of second light receiving signals obtained from the reflected light of the second distance measuring light. The received light signal used for calculating the distance information is selected. Here, the phase difference between the first ranging light and the reflected light of the first ranging light can be calculated from a plurality of first received light signals, and rough distance information to the subject can be calculated from the phase difference. It is. For this reason, the phase difference can be calculated more accurately in the same distance range as the distance information that can be calculated using the first received light signal by the second received light signal selected based on the first received light signal. Distance information representing an accurate distance can be calculated.

  Further, based on the phase difference between the first ranging light and the reflected light, the phase of the second ranging light is changed so as to be different from the phase of the first ranging light. And the second light receiving signal is acquired in a plurality of light receiving periods corresponding to the phase difference, so that it is not necessary to acquire the second light receiving signal in all the light receiving periods in which the first light receiving signal is acquired. . For this reason, distance information can be calculated quickly. Therefore, according to the present invention, accurate and high-speed distance measurement can be performed regardless of the distance to the subject.

In the distance measuring device according to the present invention, the distance measuring light emitting means may determine the minimum phase difference among the plurality of phase differences calculated for the plurality of light receiving elements as the light emission start phase of the second distance measuring light. Means for emitting the second distance measuring light earlier than the light emission start phase of the first distance measuring light;
The light reception control unit may be a unit that acquires the second light reception signal in a larger number of light reception periods as the difference between the maximum phase difference and the minimum phase difference among the plurality of phase differences is larger.

  As a result, the phase of the reflected light of the second distance measuring light that minimizes the phase difference can be matched with the phase of the modulation of the first distance measuring light, so that the second received light signal corresponding to the difference phase difference Can be easily set.

  In the distance measuring apparatus according to the present invention, the distance information calculating unit may be configured to calculate the distance information of the plurality of second received light signals based on a difference phase difference between the phase difference and the minimum phase difference. It may be a means for selecting the second received light signal used for the calculation.

  Accordingly, it is possible to set a period for acquiring the second received light signal more easily according to the differential phase difference.

  In the distance measuring device according to the present invention, the distance measuring light emitting means may be configured such that the second distance measuring light is transmitted at the same period as the modulation period of the first distance measuring light. It may be a means for emitting light for a period shorter than the light modulation period.

  Thereby, it is possible to easily control the emission of the first and second ranging light.

Further, in the distance measuring apparatus according to the present invention, the distance measuring light emitting means emits the second distance measuring light for a period of 1/4 of the modulation period of the first distance measuring light,
The light receiving control means may be means for controlling the light receiving period of the imaging means so as to be ¼ period or ½ period of the modulation period of the first distance measuring light.

  As a result, it is possible to more easily control the emission of the first and second ranging light and the reception of the reflected light of the first and second ranging light.

  In the distance measuring device according to the present invention, the distance information calculating unit may be configured to detect the second light receiving signal on the light receiving period side having a high signal level when the selected second light receiving signal extends over a plurality of light receiving periods. It may be a means used for calculating the distance information.

  Here, a large signal level means that the influence of noise due to external light is small. Therefore, the distance information can be calculated more accurately by using the second received light signal having the higher signal level for calculating the distance information.

  In the distance measuring apparatus according to the present invention, the distance information calculating unit calculates an external light signal representing an external light component based on the plurality of first light reception signals, and the selection is performed based on the external light signal. Means for correcting the second light reception signal may be used.

  Thereby, distance information can be calculated more accurately.

The distance measuring method according to the present invention includes a first distance measuring light modulated such that the intensity changes with time in a predetermined period, and a second distance light modulated in a pulse wave having a constant intensity in the predetermined period. Ranging light emitting means for switching the ranging light so that it can be switched;
An imaging means having a plurality of light receiving elements for outputting a light reception signal corresponding to the amount of received light;
A light receiving control means for controlling a light receiving period of the imaging means;
A distance measuring method in a distance measuring device comprising distance information calculating means for calculating distance information representing a distance to a subject for each of the light receiving elements based on the light receiving signal,
Emitting the first ranging light;
Obtaining a plurality of first received light signals in a plurality of light receiving periods having different phases in the modulation period of the first ranging light;
Based on the plurality of first light receiving signals, a phase difference between the first distance measuring light and the reflected light of the first distance measuring light is calculated for each light receiving element,
Based on the phase difference, the emission start phase of the second ranging light is changed to be different from the emission start phase of the first ranging light, and the second ranging light is emitted.
Obtaining a plurality of second light receiving signals in a plurality of light receiving periods according to the phase difference in the modulation period of the second ranging light;
Based on the plurality of first light reception signals, a second light reception signal used for calculating the distance information is selected.

  The distance measuring method according to the present invention may be provided as a program for causing a computer to execute the distance measuring method.

  Hereinafter, embodiments of the present invention will be described with reference to the drawings. FIG. 1 is a schematic block diagram showing the configuration of the distance measuring apparatus according to the first embodiment of the present invention. As shown in FIG. 1, the distance measuring device 1 according to the first embodiment includes an imaging unit 2.

  The imaging unit 2 includes a lens 10, a diaphragm 11, a shutter 12, a CCD 13, an analog front end (AFE) 14, and an A / D conversion unit 15.

  The lens 10 is composed of a plurality of functional lenses such as a focus lens for focusing on a subject and a zoom lens for realizing a zoom function, and its position is adjusted by a lens driving unit (not shown).

  The aperture 11 is adjusted in aperture diameter based on predetermined aperture value data by an aperture drive unit (not shown).

  The shutter 12 is a mechanical shutter and is driven according to a predetermined shutter speed.

  The CCD 13 is an image pickup device having a photoelectric surface in which a large number of light receiving devices are two-dimensionally arranged, and subject light is imaged on the photoelectric surface and subjected to photoelectric conversion to obtain a light reception signal that is an analog image pickup signal. The light receiving period of the CCD 13 is controlled by an electronic shutter drive signal given from an imaging control unit 19 described later. Further, since a filter 13A that transmits light in the wavelength range of distance measuring light, which will be described later, is disposed on the front surface of the CCD 13, the light receiving element of the CCD 13 can receive only reflected light of the distance measuring light. Here, in this embodiment, infrared light is used as distance measuring light.

  The AFE 14 performs a process for removing noise of the received light signal and a process for adjusting the gain of the received light signal (hereinafter referred to as an analog process) on the received light signal output from the CCD 13.

  The A / D converter 15 converts the received light signal that has been subjected to the analog processing by the AFE 14 into a digital signal.

  The imaging unit 2 also includes a distance measuring light source 16 for irradiating distance measuring light composed of infrared light toward the subject.

  FIG. 2 is a schematic block diagram showing the configuration of the ranging light source. As shown in FIG. 2, the distance measuring light source 16 includes a surface light source 16A in which a plurality of LEDs for emitting distance measuring light composed of infrared light are two-dimensionally arranged, and the distance measuring light emitted from the surface light source 16A is intensity-modulated. And a memory control unit 16D for reading the waveform data from the memory 16C, D / A converting the waveform data, and inputting the waveform data to the modulation unit 16B. Prepare.

  The memory control unit 16D reads predetermined waveform data in accordance with an instruction from the imaging control unit 19 described later, performs D / A conversion, and inputs the data to the modulation unit 16B. The modulator 16B modulates the intensity of the distance measuring light emitted from the surface light source 16A so as to match the waveform represented by the input waveform data.

  Here, in the present embodiment, the memory 16C stores sine wave data for intensity-modulating ranging light into a sine wave and pulse wave data for intensity-modulating ranging light into a pulse wave. . Note that the sine wave data and the pulse wave data have the same cycle, and the pulse period is a quarter of the sine wave cycle. In addition, distance measuring light whose intensity is modulated by sine wave data is referred to as first distance measuring light, and distance measuring light whose intensity is modulated by pulse wave data is referred to as second distance measuring light.

  In addition, the imaging unit 2 includes an imaging control unit 19 for controlling driving of the CCD 13, the AFE 14, and the ranging light source 16. Specifically, the imaging control unit 19 instructs the modulation unit 18 to perform modulation in accordance with an instruction from the CPU 32 and causes the ranging light irradiation unit 3 to emit the first and second ranging light, and the timing thereof. In addition, the reflected light of the distance measuring light from the subject is received, and each part of the imaging unit 2 is controlled so as to output a light reception signal corresponding to the amount of received light. Detailed control of the emission of the first and second ranging lights and the acquisition of the received light signals from the respective light receiving elements of the CCD 13 will be described later.

  In addition, the distance measuring device 1 includes an imaging condition setting unit 22, an image processing unit 23, a compression / decompression processing unit 24, a frame memory 25, a media control unit 26, an internal memory 27, and a display control unit 28.

  The shooting condition setting unit 22 stores a predetermined focal length, aperture value, and shutter speed, and outputs the focal length, aperture value, and shutter speed to the imaging unit 2 when shooting.

  The image processing unit 23 performs image processing such as gradation correction and sharpness correction on the image data of the distance image generated as described later.

  The compression / decompression processing unit 24 performs compression processing on the image data of the distance image subjected to image processing by the image processing unit 23 in a compression format such as JPEG, and generates an image file. A tag storing incidental information such as shooting date and time is added to the image file based on the Exif format or the like.

  The frame memory 25 is a working memory used when various processes including the above-described image processing are performed on the received light signal acquired by the imaging unit 2.

  The media control unit 26 accesses the recording medium 29 to control writing and reading of the distance image file.

  The internal memory 27 stores various constants set in the distance measuring device 1, a program executed by the CPU 32, and the like.

  The display control unit 28 is for displaying the image data stored in the frame memory 25 on the monitor 30 and for displaying the image recorded on the recording medium 29 on the monitor 30.

  The distance measuring device 1 includes a distance image generation unit 31 and a CPU 32.

  The distance image generation unit 31 calculates distance information D1 from the distance measuring device 1 of each point on the subject for each light receiving element on the CCD 13 using the light reception signal acquired by the imaging unit 2. Hereinafter, calculation of the distance information D1 will be described.

  The distance image generation unit 31 obtains the distance information D1 based on the time from when the intensity-modulated first ranging light is emitted until the reflected light reflected by the subject is received (that is, the flight time of light). calculate.

  FIG. 3 is a diagram for explaining the calculation of the phase difference for calculating the distance information. As shown in FIG. 3, since the intensity of the first ranging light emitted from the ranging light source 16 changes in a sine wave shape as shown by a curve K1, the received light amount of the reflected light received by a light receiving element of the CCD 13 However, the phase difference tda corresponding to the flight time of light is generated.

  The phase difference tda can be calculated using the received light amount of the reflected light obtained at a plurality of timings of the first distance measuring light. In the present embodiment, in the phase of 0, π / 2, π, 3π / 2 in the first ranging light, the light receiving period Tw corresponding to ¼ period of the first ranging light is received in pulses. The phase difference tda is calculated using the received light quantity of the reflected light.

  Here, it is assumed that the received light amounts of the reflected light received at the continuous phases of 0, π / 2, π, and 3π / 2 in the first ranging light are F1a, F2a, F3a, and F4a, respectively. It is assumed that the phase difference tda does not change during the calculation of the received light amounts F1a, F2a, F3a, and F4a, and the reflectance of the subject does not change, and the light received by each light receiving element of the CCD 13 at time t. It is assumed that the intensity is represented by A · sin (ωt + δ) + B. Here, A is the amplitude, B is the external light component, ω is the angular frequency, and δ is the phase. Accordingly, the received light amounts F1a, F2a, F3a, and F4a received by the light receiving element can be expressed as follows. The received light quantity corresponds to a received light signal output from each light receiving element in the phase of 0, π / 2, π, 3π / 2 in the distance measuring light. In addition, the calculation of the phase difference tda requires obtaining the above-described four received light amounts, that is, the four received light signals F1a, F2a, F3a, and F4a from the CCD 13, so that all the light receiving elements have four received light signals F1a. , F2a, F3a, and F4a are obtained until the first distance measuring light is emitted and the reflected light is received by the CCD 13.

F1a = A · sin (δ) + B
F2a = A · sin (π / 2 + δ) + B
F3a = A · sin (π + δ) + B
F4a = A · sin (3π / 2 + δ) + B
Here, since δ = −tda, F1a = −A · sin (tda) + B, F2a = A · cos (tda) + B, F3a = A · sin (tda) + B, F4a = −A · cos (tda ) + B, the relationship between each received light amount (light reception signal) F1a, F2a, F3a, F4a and the phase difference tda is expressed by the following equation.

tda = tan ⁻¹ {(F3a−F1a) / (F2a−F4a)} (1)
Note that the distance information D can be calculated by the following equation (2) by using the phase difference tda.

D = c · tda / (4πF) (2)
c is the speed of light, and F is the frequency (= ω / 2π).

  Here, the four light receiving signals F1a, F2a, F3a, and F4a are obtained by dividing each light receiving period by the phase of 0, π / 2, π, and 3π / 2 in the first distance measuring light in each light receiving element. However, four charge storage units are provided in each light receiving element of the CCD 13, and four light reception signals are acquired by each of the four charge storage units in one light receiving period corresponding to one cycle of the first distance measuring light. You may make it do.

  In the first embodiment, the distance image generation unit 31 emits the second distance measuring light instead of the first distance measuring light after calculating the phase difference tda. Here, since the second distance measuring light has the same period as the first distance measuring light and the light emission period is ¼ of the first distance measuring light, that is, Tw, the reflected light is also a pulse of the period Tw. Light. The reflected light of the second distance measuring light also has a phase difference in the same manner as the reflected light of the first distance measuring light.

  The distance image generation unit 31 calculates the minimum phase difference t1 among the phase differences tda calculated for all the light receiving elements, and outputs the minimum phase difference t1 to the imaging unit 2. The imaging control unit 19 of the imaging unit 2 emits the second ranging light from the ranging light source 16 by advancing the emission start phase by the minimum phase difference t1. That is, when the light emission start phase is not changed, the second distance measuring light is emitted at the same light emission start phase as the light emission start phase of the first distance measuring light, as shown by the broken line in FIG. By advancing the light emission start phase by the minimum phase difference t1, the second distance measuring light is emitted as shown by the solid line in FIG.

  Further, the distance image generation unit 31 calculates the maximum phase difference t2 of the phase difference tda, calculates a difference phase difference tr (= t2−t1) between the maximum phase difference t2 and the minimum phase difference t1, and outputs the difference to the imaging unit 2. To do. The imaging control unit 19 of the imaging unit 2 has the same light reception period as the reflected light of the first ranging light (that is, the first ranging light) in one cycle of the second ranging light emission according to the differential phase difference tr. Of the light receiving periods Tw) corresponding to the phases 0, π / 2, π, and 3π / 2 of the modulation period of the ranging light, it is set in which light receiving period the reflected light is received.

  FIG. 4 is a diagram for explaining the setting of the light receiving period. The second ranging light has a light emission start phase earlier than the first ranging light by the minimum phase difference t1 calculated using the first ranging light. For this reason, the reflected light that is received earliest is shifted in phase by the minimum phase difference t1 from the second ranging light, so that the phase of the reflected light is the first ranging at 0 phase as shown in FIG. This corresponds to a period Tw corresponding to a quarter cycle of light.

  On the other hand, since the differential phase difference tr has a value less than one modulation period of the first ranging light, the reflected light of the second ranging light has a period corresponding to one modulation period of the first ranging light. It is sufficient to receive the light at. Therefore, it can be seen that light should be received in the light receiving period Tw corresponding to any phase of 0, π / 2, π, 3π / 2 of the modulation period of the first distance measuring light according to the difference phase difference tr. It will be.

  Specifically, when tr ≦ T / 4 (T is one modulation period of the first distance measuring light), the phase of the reflected light of the second distance measuring light is 0 to π. It is only necessary to receive the reflected light in the two light receiving periods Tw of 0 and π / 2. When T / 4 <tr ≦ T / 2, the phase of the reflected light of the second ranging light is 0-3π / 2 as shown in the case of the differential phase difference tr1 in FIG. Therefore, it is only necessary to receive the reflected light in the three light receiving periods Tw of 0, π / 2, and π. In the case of T / 2 <tr ≦ T, the phase of the reflected light of the second distance measuring light is 0-2π as shown in the case of the differential phase difference tr2 in FIG. , Π / 2, π, and 3π / 2, it is only necessary to receive the reflected light in all the light receiving periods Tw.

  The light reception obtained by receiving the reflected light of the second ranging light in the light receiving period Tw corresponding to the phase of 0, π / 2, π, 3π / 2 of the modulation period of the first ranging light. The signals are light reception signals F1b, F2b, F3b, and F4b.

  Further, the distance image generation unit 31 calculates a differential phase difference ts (ts = tda-1) between the phase difference tda and the minimum phase difference t1 for each light receiving element, and based on the differential phase difference ts, the light reception signal F1b, Of F2b, F3b, and F4b, the received light signal used for calculating the phase difference tdb is selected. That is, if the phase difference tda is within Tw, the reflected light of the second distance measuring light exists between the phases of 0 to π of the first distance measuring light, so that the light reception signals F1b and F2b are selected. . Then, the phase difference tdb is calculated by the following equation (3).

tdb = Tw × F2b / (F1b + F2b) (3)
If the differential phase difference ts is greater than Tw and within 2 Tw, the reflected light of the second distance measuring light exists between the phases of π / 2 to 3π / 2 of the first distance measuring light. The generation unit 31 selects the light reception signals F2b and F3b. Then, the phase difference tdb is calculated by the following equation (4).

tdb = Tw + Tw × F3b / (F2b + F3b) (4)
If the differential phase difference ts is larger than 2Tw and within 3Tw, the reflected light of the second distance measuring light exists between the phases of π to 2π (that is, 0) of the first distance measuring light. The generation unit 31 selects the light reception signals F3b and F4b. Then, the phase difference tdb is calculated by the following equation (5).

tdb = 2Tw + Tw × F4b / (F3b + F4b) (5)
Further, if the differential phase difference ts is greater than 3Tw and within 4Tw, the reflected light of the second ranging light is between 3π / 2 and π / 2 (next period) of the first ranging light. Therefore, the distance image generation unit 31 selects the light reception signals F4b and F1b. Then, the phase difference tdb is calculated by the following equation (6).

tdb = 3Tw + Tw × F1b / (F4b + F1b) (6)
Then, distance information D1 representing the distance to the subject is calculated for each light receiving element by the following equation (7) using the phase difference tdb.

D1 = c × (tdb + t1) / 2 (7)
C is the speed of light.

  Furthermore, the distance image generation unit 31 generates a distance image S1 using the distance information D1 calculated for each light receiving element as described above as the pixel value of each pixel.

  When the differential phase difference is tr ≦ T / 4, only the two light reception signals F1b and F2b are acquired. However, since ts ≦ Tw, the phase difference tdb is always calculated by the equation (3). When the differential phase difference is T / 4 <tr ≦ T / 2, only three light reception signals F1b, F2b, and F3b are acquired. However, since ts ≦ 2Tw, the expressions (3) and (4) are always used. Thus, the phase difference tdb is calculated.

  The CPU 32 controls each unit of the distance measuring device 1 according to a signal from the input / output unit 33.

  The data bus 34 is connected to each unit constituting the distance measuring device 1 and the CPU 32, and exchanges various data and various information in the distance measuring device 1.

  Next, processing performed in the first embodiment will be described. 5 and 6 are flowcharts showing the processing performed in the first embodiment.

  The CPU 32 starts processing when a shooting instruction is given, and the imaging unit 2 emits first ranging light from the ranging light source 16 toward the subject in response to the instruction from the CPU 32 (step ST1). The reflected light from the subject of the ranging light is received at the continuous phase of 0, π / 2, π, 3π / 2 in the first ranging light, and four received light signals F1a, F2a, F3a, and F4a are obtained. (Step ST2). Next, the distance image generation unit 31 calculates the phase difference tda for each light receiving element from the four light receiving signals F1a, F2a, F3a, and F4a according to the above equation (1) (step ST3). Further, the distance image generation unit 31 calculates a difference phase difference tr between the maximum phase difference t2 and the minimum phase difference t1 of the phase difference tda (step ST4).

  Then, the imaging control unit 19 of the imaging unit 2 sets the emission start phase of the second ranging light so as to be earlier than the first ranging light by the minimum phase difference t1 (step ST5), and the differential phase difference The range of tr is determined (step ST6).

  In the case of tr ≦ T / 4, the imaging control unit 19 sets the light receiving period of each light receiving element of the CCD 13 so as to receive the reflected light in the light receiving period Tw having a phase of 0 and π / 2 (step ST7). Then, the second ranging light is emitted from the ranging light source 16 toward the subject (step ST8), and the reflected light of the second ranging light from the subject is set to 0, π / corresponding to the set light receiving period. Light is received in phase 2, and two light reception signals F1b and F2b are acquired (step ST9).

  In the case of T / 4 <tr ≦ T / 2, the imaging control unit 19 receives the reflected light in the light receiving periods Tw having the phases of 0, π / 2, and π, so that the light receiving periods of the respective light receiving elements of the CCD 13 are received. Is set (step ST10). Then, the second ranging light is emitted from the ranging light source 16 toward the subject (step ST8), and the reflected light of the second ranging light from the subject is set to 0, π / corresponding to the set light receiving period. Light is received at the phase of 2 and π, and three light reception signals F1b, F2b, and F3b are obtained (step ST11).

  In the case of T / 2 <tr ≦ T, the imaging control unit 19 receives each reflected light of the CCD 13 so as to receive the reflected light in all the light receiving periods Tw whose phases are 0, π / 2, π, and 3π / 2. The light receiving period of the element is set (step ST12). Then, the second ranging light is emitted from the ranging light source 16 toward the subject (step ST8), and the reflected light of the second ranging light from the subject is set to 0, π / corresponding to the set light receiving period. Light is received at a phase of 2, π, and 3π / 2, and four received light signals F1b, F2b, F3b, and F4b are obtained (step ST13).

  Subsequently, the distance image generation unit 31 calculates the difference phase difference ts between the phase difference tda and the minimum phase difference t1 for each light receiving element (step ST14), and determines the range of the difference phase difference ts (step ST15).

  In the case of ts ≦ Tw, the phase difference tdb is calculated by the above equation (3) (step ST16). In the case of Tw <ts ≦ 2Tw, the phase difference tdb is calculated by the above equation (4) (step ST17). In the case of 2Tw <ts ≦ 3Tw, the phase difference tdb is calculated by the above equation (5) (step ST18). When 3Tw <ts ≦ 4Tw, the phase difference tdb is calculated by the above equation (6) (step ST19).

  Next, the distance image generation unit 31 calculates the distance information D1 by the above formula (7) (step ST20), and generates a distance image S1 having the distance information D1 as the pixel value of each pixel (step ST21). Then, the media control unit 26 records the image data of the distance image S1 on the recording medium 29 (step ST22), and the process ends.

  Here, when using the first ranging light that is modulated so that the intensity varies with time, such as a sine wave, ranging can be performed with a relatively long range, depending on the phase of the modulation. The intensity of reflected light is reduced. For example, in the phase of π / 2 shown in FIG. 3, the intensity of the reflected light is very small. For this reason, when the first ranging light is used, the S / N of the received light signal is lowered due to the influence of external light, so the accuracy of ranging is not so high.

  On the other hand, when using the second ranging light whose intensity is modulated in a pulse shape with a constant intensity, the intensity of the reflected light is constant, so that the S / N is hardly lowered and the ranging can be performed with high accuracy. . However, since the range in which distance measurement can be performed is limited by the pulse width, distance measurement can be performed only in a limited range.

  According to the first embodiment, on the basis of the plurality of light reception signals F1a, F2a, F3a, and F4a obtained from the reflected light of the first distance measuring light, the plurality of light obtained from the reflected light of the second distance measuring light. Among the second light reception signals F1b, F2b, F3b, and F4b, a light reception signal used for calculating the distance information D1 is selected. Here, the phase difference tda between the first distance measurement light and the reflected light of the first distance measurement light can be known from the plurality of first light reception signals F1a, F2a, F3a, and F4a. The phase difference tda can be used to calculate rough distance information to the subject, and the second received light signals F1b, F2b, F3b, and F4b used to calculate the distance information D1 based on the differential phase difference ts obtained from the phase difference tda are obtained. By selecting, the distance information can be calculated more accurately in the same distance range as the distance information obtained from the phase difference tda. Therefore, according to the first embodiment, accurate distance measurement can be performed regardless of the distance to the subject.

  In addition, the minimum phase difference t1 is calculated from the reflected light of the first distance measuring light, and the emission start phase of the second distance measuring light is advanced from the first distance measuring light by the minimum phase difference t1 to advance the second distance measuring light. And the second light reception signal is acquired in a plurality of light reception periods corresponding to the difference phase difference tr between the maximum phase difference t2 and the minimum phase difference t1, and therefore the light reception period of the first light reception signal is acquired. In all cases, it is not necessary to acquire the second received light signal. For example, when the reflected light of the second distance measuring light is received in all phases, it is necessary to obtain the received light signals for 8 phases together with the reception of the first distance measuring light. However, when ts ≦ Tw When Tw <ts ≦ 2Tw, it is only necessary to acquire light reception signals for 6 phases and 7 phases, respectively.

  Therefore, according to the present embodiment, accurate and high-speed distance measurement can be performed regardless of the distance to the subject.

  Next, a second embodiment of the present invention will be described. In the second embodiment, only the processing performed in the first embodiment is different, and the configuration of the apparatus is the same as that of the first embodiment, and thus detailed description of the configuration is omitted. Here, the received light signals F1b, F2b, F3b, and F4b obtained from the reflected light of the second distance measuring light extend over two light receiving periods. However, since the reflected light is pulsed light, the signal in each light receiving period. The level of will be different. For example, as shown in FIG. 7, when the light reception signals F1b and F2b extend over two light reception periods, the light reception signal F1b has a higher signal level. The second embodiment is different from the first embodiment in that the phase difference tdb is calculated using the light reception signal in the light reception period on the side where the signal level is large.

  FIG. 8 is a flowchart showing processing performed in the second embodiment. In the second embodiment, only processes after step ST14 in the first embodiment are different, and therefore, only processes after step ST14 in the first embodiment will be described. Subsequent to step ST14, the distance image generation unit 31 determines the range of the differential phase difference ts (step ST31).

  In the case of ts ≦ Tw, it is further determined whether or not F1b ≦ F2b is satisfied (step ST32). If step ST32 is affirmed, the phase difference tdb is calculated by the above equation (3) (step ST33). If step ST32 is negative, the phase difference tdb is calculated by the following equation (8) (step ST34).

tdb = Tw × {1−F1b / (F1b + F2b)} (8)
In the case of Tw <ts ≦ 2Tw, it is further determined whether or not F2b ≦ F3b (step ST35). If step ST35 is affirmed, the phase difference tdb is calculated by the above equation (4) (step ST36). If step ST35 is negative, the phase difference tdb is calculated by the following equation (9) (step ST37).

tdb = Tw + Tw × {1−F2b / (F2b + F3b)} (9)
If 2Tw <ts ≦ 3Tw, it is further determined whether or not F3b ≦ F4b is satisfied (step ST38). If step ST38 is positive, the phase difference tdb is calculated by the above equation (5) (step ST39). If step ST38 is negative, the phase difference tdb is calculated by the following equation (10) (step ST40).

tdb = 2Tw + Tw × {1−F3b / (F3b + F4b)} (10)
If 3Tw <ts ≦ 4Tw, it is further determined whether or not F4b ≦ F1b (step ST41). If step ST41 is affirmed, the phase difference tdb is calculated by the above equation (6) (step ST42). . If step ST42 is negative, the phase difference tdb is calculated by the following equation (11) (step ST43).

tdb = 3Tw + Tw × {1−F4b / (F4b + F1b)} (11)
Next, the distance image generation unit 31 performs the processing after step ST20 in the first embodiment, and ends the processing.

  Here, a large signal level means that the influence of noise due to external light is small. Therefore, the distance information D1 can be calculated more accurately by using the second received light signal having the higher signal level for calculating the distance information D1.

  Next, a third embodiment of the present invention will be described. In the third embodiment, only the processing performed in the first embodiment is different, and the configuration of the apparatus is the same as that of the first embodiment, and thus detailed description of the configuration is omitted. Here, the reflected light of the first and second distance measuring lights includes an external light component. Since the external light component is superimposed on the reflected light as shown by the hatched lines in FIGS. 9A and 9B, the light reception signal includes the external light component.

  Since the calculation of the phase difference tda from the light reception signal of the reflected light of the first distance measuring light is performed by the above equation (1), the influence of the external light component is removed. However, the calculation of the phase difference tdb from the light reception signal of the reflected light of the second distance measuring light is performed by the above formulas (3) to (6), and therefore includes the influence of the external light component. Yes. In the third embodiment, the phase difference tdb is calculated by removing the influence of the external light component.

Here, the light reception signal for one cycle of the reflected light of the first ranging light is F1a + F2a + F3a + F4a. The amplitude A of the reflected light of the first ranging light is calculated by A = √ {(F1a−F3a) ² + (F2a−F4a) ² }. As shown in FIG. 9 (a), the amplitude A is a rectangle having a quarter period of the reflected light of the first distance measuring light as one side and the maximum value of the brightness of the reflected light excluding the external light component as the other side. Therefore, the average value Am of the amplitude A for one period of the reflected light of the first distance measuring light is Am = (A × 4) / 2. Accordingly, the external light component k ′ for one period of the reflected light of the first ranging light is calculated by k ′ = (F1a + F2a + F3a + F4a) − (A × 4) / 2. On the other hand, since the phase of each received light signal is ¼ period of the reflected light, the external light component k can be calculated as shown in the following formula (12) by setting the external light component k ′ to ¼. .

k = {(F1a + F2a + F3a + F4a) − (A × 4) / 2} / 4 (12)
The distance image generation unit 31 calculates the external light component k by the above equation (12), and subtracts the external light component k from the received light signals F1b, F2b, F3b, and F4b of the reflected light of the second distance measuring light. The phase difference tdb is calculated using the received light signals F1b ′, F2b ′, F3b ′, and F4b ′ obtained by the above.

  FIG. 10 is a flowchart showing processing performed in the third embodiment. In the third embodiment, since only the processes between steps ST9, ST11, ST13 and step ST14 in the first embodiment are different, here, steps ST9, ST11, ST13 in the first embodiment and Only the processing between step ST14 will be described.

  Subsequent to steps STST9, ST11, and ST13, the distance image generation unit 31 calculates an external light component k by the above equation (12) (step ST41). Then, the light reception signals F1b, F2b, F3b, and F4b are corrected by the external light component k (step ST42), and the process proceeds to step ST14.

  In the third embodiment, the processes of steps ST16, ST17, ST18, and ST19 in the first embodiment are performed by the received light signals F1b ′, F2b ′, F3b ′, and F4b ′ corrected by the external light component k. Will be done.

  Thereby, the influence of an external light component can be removed and a distance image can be generated with higher accuracy.

  In the third embodiment, the external light component is removed in the first embodiment. Of course, the external light component can also be removed in the second embodiment.

  Further, in the first to third embodiments, the phase of 0 in the modulation period of the first ranging light is used as a reference, but the phase is shifted by π / 2 from the reference phase and the reference phase with a non-zero phase as a reference. The reflected light may be received at the phase, the phase shifted by π from the reference phase, and the phase shifted by 3π / 2 from the reference phase. Further, the phase shift for acquiring the received light signal is not limited to π / 2.

  In the first to third embodiments, the first ranging light corresponding to the four phases 0, π / 2, π, and 3π / 2 in the modulation period of the first ranging light is used. The light receiving signals F1a, F2a, F3a, F4a, F1b, F2b, F3b, and F4b are acquired in four light receiving periods Tw that are ¼ of one period, but 0, π / 2 in the modulation period of the ranging light, The phase difference can also be calculated by acquiring light reception signals in three light reception periods 2Tw corresponding to the three phases of π, which is ½ of one cycle of the first ranging light. Hereinafter, this will be described as a fourth embodiment.

  FIG. 11 is a diagram for explaining the calculation of the phase difference in the fourth embodiment. As shown in FIG. 11, in the fourth embodiment, in the three phases of 0, π / 2, and π in the modulation period of the first ranging light, the light reception period 2Tw reflected light that is half the modulation period is received. Thus, the light receiving timing of the light receiving element is controlled. In addition, let the received light quantity acquired by this be F1c, F2c, and F3c.

  The received light amount F1c is a received light signal in the period of 0 to π of the ranging light modulation period, the received light amount F2c is a received light signal in the period of π / 2 to 3π / 2, and the received light amount F3c is π to 2π. F1c, F2c, and F3c are also used as reference symbols for the light reception signals in order to correspond to the light reception signals in the period.

  Further, the received light amount of the curve K2 obtained in the phase of 0 to π / 2, π / 2 to π, π to 3π / 2, 3π / 2 to 2π in the curve K1 is the received light amount F1a in the first embodiment. , F2a, F3a, and F4a. Accordingly, since F1c = F1a + F2a, F2c = F2a + F3a, and F3c = F3a + F4a, the following relationship is established.

F2c-F1c = F3a-F1a
F2c-F3c = F2a-F4a
Here, since the phase difference tdc corresponding to the phase difference tda can be calculated by the above equation (1), if the above relationship is substituted into the equation (1),
tdc = tan ⁻¹ {(F2c−F1c) / (F2c−F3c)} (13)
It becomes. Therefore, the phase difference tdc corresponding to the phase difference tda can also be calculated from the received light signals F1c, F2c, and F3c acquired in the three phases by the equation (13).

  In the fourth embodiment, the calculation of the differential phase difference tr and the setting of the light emission start phase of the second distance measuring light are performed in the same manner as in the first embodiment.

  Regarding the light receiving period of the second light receiving element, the differential phase difference tr is a value less than one cycle of the first distance measuring light, so the reflected light of the second distance measuring light is the first distance measuring light. It is sufficient to receive light in a period corresponding to one cycle. Accordingly, it can be determined whether light reception should be performed in the light reception period 2Tw corresponding to the phase of 0, π / 2, or π of the modulation period of the first distance measuring light according to the difference phase difference tr.

  That is, in the case of tr ≦ T / 2 (T is one cycle of the first distance measuring light), the phase of the reflected light of the second distance measuring light is 0 to π. It is sufficient to receive the reflected light during the two light receiving periods 2Tw. In addition, when T / 2 <tr, the phase of the reflected light of the second distance measuring light is 0 to 2π, so that the reflected light is reflected in all light receiving periods 2Tw of 0, π / 2, and π. What is necessary is just to receive light.

  In this way, the imaging control unit 19 of the imaging unit 2 determines the light receiving period 2Tw of the reflected light of the second ranging light according to the differential phase difference tr. Note that the light reception signal obtained by receiving the reflected light of the second distance measuring light in the light receiving period 2Tw corresponding to the phase of 0, π / 2, π of the modulation period of the first distance measuring light is the light reception signal. Let F1d, F2d, and F3d.

  Further, the distance image generation unit 31 calculates a differential phase difference ts (ts = tdc-1) between the phase difference tdc and the minimum phase difference t1, and based on the differential phase difference ts, the light reception signals F1d, F2d, and F3bd Among them, the light reception signal used for calculating the phase difference tdd is selected. That is, if the differential phase difference ts is within Tw, the reflected light of the second distance measuring light exists between the phases of 0 to π of the first distance measuring light, so the light reception signals F1d and F2d are selected. To do. Then, the phase difference tdd is calculated by the following equation (14).

tdd = Tw × F2d / F1d (14)
If the differential phase difference ts is larger than Tw and within 2 Tw, the reflected light of the second distance measuring light exists between the phases of π / 2 to 3π / 2 of the first distance measuring light. Select F1d and F2d. Then, the phase difference tdd is calculated by the following equation (15).

tdd = Tw + Tw × (1−F1d / F2d) (15)
If the differential phase difference ts is greater than 2Tw and within 3Tw, the reflected light of the second distance measuring light exists between the phases of π to 2π (that is, 0) of the first distance measuring light. F2d and F3d are selected. Then, the phase difference tdd is calculated by the following equation (16).

tdd = 2Tw + Tw × (1−F2d / F3d) (16)
Further, if the differential phase difference ts is greater than 3Tw and within 4Tw, the reflected light of the second ranging light is between 3π / 2 and π / 2 (next period) of the first ranging light. Since it exists, the light reception signals F3d and F1d are selected. Then, the phase difference tdd is calculated by the following equation (17).

tdd = 3Tw + Tw × F1d / (F3d + F1d) (17)
Then, using the phase difference tdd, distance information D1 representing the distance to the subject is calculated for each light receiving element by the above equation (7).

  When the differential phase difference is tr ≦ T / 2, only the two light reception signals F1d and F2d are acquired. However, since ts ≦ 2Tw, the phase difference tdd is always expressed by the equations (14) and (15). Calculated.

  Next, processing performed in the fourth embodiment will be described. 12 and 13 are flowcharts showing the processing performed in the fourth embodiment. The CPU 32 starts processing when a shooting instruction is issued, and the imaging unit 2 emits first ranging light from the ranging light source 16 toward the subject according to the instruction from the CPU 32 (step ST51). The reflected light from the subject of the distance measuring light is received at the continuous 0, π / 2, and π phases in the first distance measuring light, and three received light signals F1c, F2c, and F3c are obtained (step ST52). Next, the distance image generation unit 31 calculates the phase difference tdc for each light receiving element from the three light receiving signals F1c, F2c, and F3c according to the above equation (13) (step ST53). Further, the distance image generation unit 31 calculates a difference phase difference tr between the maximum phase difference t2 and the minimum phase difference t1 of the phase difference tdc (step ST54).

  Then, the imaging control unit 19 of the imaging unit 2 sets the emission start phase of the second ranging light so as to be earlier than the first ranging light by the minimum phase difference t1 (step ST55), and the differential phase difference The range of tr is determined (step ST56).

  In the case of tr ≦ T / 2, the imaging control unit 19 sets the light receiving period of each light receiving element of the CCD 13 so as to receive the reflected light in the light receiving period 2Tw having a phase of 0 and π / 2 (step ST57). Then, the second ranging light is emitted from the ranging light source 16 toward the subject (step ST58), and the reflected light of the second ranging light from the subject is set to 0, π / corresponding to the set light receiving period. Light is received in phase 2, and two light reception signals F1d and F2d are acquired (step ST59).

  When T / 2 <tr, the imaging control unit 19 sets the light receiving period of each light receiving element of the CCD 13 so as to receive the reflected light in the light receiving period 2Tw having the phases of 0, π / 2, and π ( Step ST60). Then, the second ranging light is emitted from the ranging light source 16 toward the subject (step ST58), and the reflected light of the second ranging light from the subject is set to 0, π / corresponding to the set light receiving period. Light is received at the phase of 2 and π, and three light reception signals F1d, F2d, and F3d are obtained (step ST61).

  Subsequently, the distance image generation unit 31 calculates a differential phase difference ts between the phase difference tdc and the minimum phase difference t1 (step ST62), and determines a range of the differential phase difference ts (step ST63).

  When ts ≦ Tw, the phase difference tdd is calculated by the above equation (14) (step ST64). In the case of Tw <ts ≦ 2Tw, the phase difference tdd is calculated by the above equation (15) (step ST65). In the case of 2Tw <ts ≦ 3Tw, the phase difference tdd is calculated by the above equation (16) (step ST66). When 3Tw <ts ≦ 4Tw, the phase difference tdd is calculated by the above equation (17) (step ST67).

  Next, the distance image generation unit 31 calculates distance information D1 by the above equation (7) (step ST68), and generates a distance image S1 having the distance information D1 as the pixel value of each pixel (step ST69). Then, the media control unit 26 records the image data of the distance image S1 on the recording medium 29 (step ST70), and ends the process.

  In the fourth embodiment, as in the third embodiment, the external light component k is calculated from the light reception signals F1c, F2c, and F3c, and the light reception signals F1d, F2d, and F3d are corrected by the external light component k. Thus, the phase difference tdd may be calculated. In this case, the external light component k is calculated by the following equation (18).

k = (F1c + F3c) / 2
−√ {(F1c−F2c) ² + (F2c−F3c) ² } (18)
In each of the above embodiments, the first distance measuring light is modulated by a sine wave. However, any modulation may be performed as long as it modulates at a constant cycle such as a triangular wave or a pulse wave. Good.

  In each of the above embodiments, the distance image is generated in the distance measuring device 1. However, the distance image generating unit 31 is provided outside the device 1, and the received light signal is input from the input / output unit 33 to the external distance image generating unit. The distance image may be generated by outputting to 31.

  Although the distance measuring device according to the embodiment of the present invention has been described above, the computer functions as a unit corresponding to the distance image generation unit 31 as shown in FIGS. A program for performing a simple process is also one embodiment of the present invention. A computer-readable recording medium in which such a program is recorded is also one embodiment of the present invention.

1 is a schematic block diagram showing the configuration of a distance measuring device according to a first embodiment. Schematic block diagram showing the configuration of the ranging light source configuration The figure for demonstrating calculation of the phase difference in 1st Embodiment. Diagram for explaining the setting of the light reception period The flowchart which shows the process performed in 1st Embodiment (the 1) The flowchart which shows the process performed in 1st Embodiment (the 2) The figure which shows the light reception signal over two light reception periods The flowchart which shows the process performed in 2nd Embodiment. Diagram for explaining external light components The flowchart which shows the process performed in 3rd Embodiment The figure for demonstrating calculation of the phase difference in 4th Embodiment The flowchart which shows the process performed in 4th Embodiment (the 1) The flowchart which shows the process performed in 4th Embodiment (the 2)

Explanation of symbols

DESCRIPTION OF SYMBOLS 1 Distance measuring device 2 Imaging part 13 CCD
16 Ranging light source 19 Imaging control unit 31 Distance image generation unit 32 CPU

Claims (9)

The first distance measuring light modulated so that the intensity varies with time in a predetermined period and the second distance measuring light modulated in a pulse wave having a constant intensity in the predetermined period can be switched. Ranging light emitting means for
An imaging means having a plurality of light receiving elements for outputting a light reception signal corresponding to the amount of received light;
A light receiving control means for controlling a light receiving period of the imaging means;
Distance information calculating means for calculating distance information representing a distance to a subject for each light receiving element based on the light receiving signal;
The first ranging light is emitted, a plurality of first received light signals are acquired in a plurality of light receiving periods having different phases in a modulation period of the first ranging light, and the first received light signals are Based on this, a phase difference between the first distance measuring light and the reflected light of the first distance measuring light is calculated for each light receiving element, and emission of the second distance measuring light is started based on the phase difference. A phase is changed so as to be different from the light emission start phase of the first distance measuring light, the second distance measuring light is emitted, and a plurality of signals corresponding to the phase difference in the modulation period of the second distance measuring light are emitted. A plurality of second light reception signals are acquired during the light reception period, and the distance measurement light emission is performed so as to select a second light reception signal used for calculating the distance information based on the plurality of first light reception signals. And a control means for controlling the imaging means, the light reception control means, and the distance information calculation means. Distance measuring apparatus according to claim. The ranging light emitting unit calculates a minimum phase difference of the plurality of phase differences calculated for the plurality of light receiving elements from the emission starting phase of the first ranging light. A means for emitting the second distance measuring light earlier,
The light reception control means is means for acquiring the second light reception signal in a larger number of light reception periods as the difference phase difference between the maximum phase difference and the minimum phase difference among the plurality of phase differences is larger. The distance measuring apparatus according to claim 1.   The distance information calculation means selects a second light reception signal used for calculating the distance information from the plurality of second light reception signals based on a differential phase difference between the phase difference and the minimum phase difference. The distance measuring apparatus according to claim 1, wherein the distance measuring apparatus is a means for performing the operation.   The distance measuring light emitting means emits the second distance measuring light at the same period as the modulation period of the first distance measuring light and for a period shorter than the modulation period of the first distance measuring light. The distance measuring device according to any one of claims 1 to 3, wherein The distance measuring light emitting means is a means for emitting the second distance measuring light for a period of 1/4 of the modulation period of the first distance measuring light,
The light receiving control means is a means for controlling the light receiving period of the reflected light of the second distance measuring light to be ¼ period or ½ period of the modulation period of the first distance measuring light. The distance measuring device according to claim 1, wherein   The distance information calculation means is means for using the second light reception signal on the light reception period side having a high signal level for the calculation of the distance information when the selected second light reception signal extends over a plurality of light reception periods. The distance measuring apparatus according to claim 1, wherein:   The distance information calculation unit is a unit that calculates an external light signal representing an external light component based on the plurality of first light reception signals, and corrects the selected second light reception signal based on the external light signal. The distance measuring device according to claim 1, wherein The first distance measuring light modulated so that the intensity varies with time in a predetermined period and the second distance measuring light modulated in a pulse wave having a constant intensity in the predetermined period can be switched. Ranging light emitting means for
An imaging means having a plurality of light receiving elements for outputting a light reception signal corresponding to the amount of received light;
A light receiving control means for controlling a light receiving period of the imaging means;
A distance measuring method in a distance measuring device comprising distance information calculating means for calculating distance information representing a distance to a subject for each of the light receiving elements based on the light receiving signal,
Emitting the first ranging light;
Obtaining a plurality of first received light signals in a plurality of light receiving periods having different phases in the modulation period of the first ranging light;
Based on the plurality of first light receiving signals, a phase difference between the first distance measuring light and the reflected light of the first distance measuring light is calculated for each light receiving element,
Based on the phase difference, the emission start phase of the second ranging light is changed to be different from the emission start phase of the first ranging light, and the second ranging light is emitted.
Obtaining a plurality of second light receiving signals in a plurality of light receiving periods according to the phase difference in the modulation period of the second ranging light;
2. A distance measuring method, comprising: selecting a second received light signal used for calculating the distance information based on the plurality of first received light signals. The first distance measuring light modulated so that the intensity varies with time in a predetermined period and the second distance measuring light modulated in a pulse wave having a constant intensity in the predetermined period can be switched. Ranging light emitting means for
An imaging means having a plurality of light receiving elements for outputting a light reception signal corresponding to the amount of received light;
A light receiving control means for controlling a light receiving period of the imaging means;
A program for causing a computer to execute a distance measuring method in a distance measuring device including distance information calculating means for calculating distance information representing a distance to a subject for each of the light receiving elements based on the light receiving signal,
A procedure for emitting the first distance measuring light;
Obtaining a plurality of first received light signals in a plurality of light receiving periods having different phases in the modulation period of the first ranging light;
Calculating a phase difference between the first ranging light and the reflected light of the first ranging light for each of the light receiving elements based on the plurality of first received light signals;
Changing the light emission start phase of the second distance measuring light based on the phase difference to be different from the light emission start phase of the first distance measuring light, and emitting the second distance measuring light;
Obtaining a plurality of second light receiving signals in a plurality of light receiving periods according to the phase difference in the modulation period of the second ranging light;
And a procedure for selecting a second light reception signal used for calculating the distance information based on the plurality of first light reception signals.

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