This application is a National Stage of Application No. PCT/JP2018/010755 filed Mar. 19, 2018 the disclosure of which is incorporated herein in its entirety by reference.
The present invention relates to an object detection apparatus for emitting a radio wave to a detection target and recognizing or identifying the presence of the detection target by detecting a radio wave reflected or emitted from the target, and an object detection method, and further relates to a computer-readable recording medium where a program for realizing these is recorded.
Radio waves (microwaves, millimeter waves, terahertz waves, and the like) are superior to light in terms of their ability to pass through objects. Apparatus that utilize this penetration ability of radio waves in order to visualize articles under clothes or in a bag to perform inspection have been put into practical use. Also, remote sensing technology, which utilizes the penetration ability of radio waves in order to visualize the ground surface from satellites or aircraft by the radio waves passing through clouds, has also been put into practical use.
Several systems have been proposed in imaging devices (object detection apparatus) using radio waves. One of these is an array antenna system, which is shown in a concept diagram in
Also, as shown in
The transmitter 211 emits an RF signal (radio wave) 213 from the transmission antenna 212 toward detection targets 2041, 2042, . . . , 204K (where K is the number of targets). The RF signal (radio wave) 213 is reflected at the detection targets 2041, 2042, . . . , 204K, thus respectively generating reflection waves 2031, 2032, . . . , 203K. The generated reflection waves 2031, 2032, . . . , 203K are received by the receiving antennas 2021, 2022, . . . , 202N.
The receiver 201 calculates the intensity of the radio waves reflected from the detection targets 2041, 2042, . . . , 204K based on the received reflection waves 2031, 2032, . . . , 203K. By converting the distribution of that radio wave intensity to an image, an image of the detection targets 2041, 2042, . . . , 204K can be obtained.
In the array antenna system, as shown in
The phase shifters 2061, 2062, . . . , 206N and the adder 207 may be implemented with analog circuits, or may be implemented with digital processing by software. In the array antenna system, the directivity of the array antennas is controlled according to setting of the phase rotations Φ1, Φ2, . . . , ΦN by the phase shifters 2061, 2062, . . . , 206N. When the directivity of the receiving antennas 202 is g(θ), and the amplitude and the phase of an incoming wave 208n (where n=1, 2, . . . , N) received by a receiving antenna 202n are an and θn, respectively, the directivity E(θ) of the array antennas is calculated by the following Formula (1).
Note that the directivity component AF(θ) obtained by removing the directivity g(θ) of the receiving antenna 202 from the directivity E(θ) of the array antenna in Formula (1) is called an array factor. The array factor AF(θ) represents the effects of directivity due to the formation of the array antenna. The signal received by the receiving antenna 202n (where n=1, 2, . . . , N) is expressed as g(θ)anexp(φn). A signal g(θ)anexp(jφn)exp(jφn) obtained by receiving the phase rotation Φn of the phase shifter 206n is added across n=1, 2, . . . , N by the adder 207, and this signal is obtained as the directivity E(θ) of Formula (1).
When the receiving antenna 202n (where n=1, 2, . . . , N) receives the incoming wave 208n with an incidence angle θ, the phase φn of the incoming wave 208n is given as −2π·n·d·sin θ/λ (where n=1, 2, . . . , N). Here, d is the interval of the receiving antenna 202n (where n=1, 2, . . . , N), and λ is the wavelength of the incoming waves 2081, 2082, . . . , 208N.
In Formula (1), when the amplitude an is constant regardless of n, if the phase rotation Φn (where n=1, 2, . . . , N) of the phase shifter 206n is set to be equal to the phase φn of the incoming wave 208n, the array factor AF(θ) becomes maximum in the direction of the angle θ. In other words, the directivity of the array antenna is controlled by the phase rotation Φn of the phase shifter 206n.
Examples of a radio wave imaging device using an array antenna system are disclosed in Patent Documents 1 to 3.
In the array antenna systems disclosed in Patent Documents 1 and 2, the phase shifters 2061, 2062, . . . , 206N are built into the receiver 201, and connected to the receiving antennas 2021, 2022, . . . , 202N. The directivity of the receiving array antenna formed by the receiving antennas 2021, 2022, . . . , 202N is controlled by the phase shifters 2061, 2062, . . . , 206N.
That is, by changing the directivity of the receiving array antennas (2021, 2022, . . . , 202N) formed in a beam shape, and directing the directivity beam of the receiving array antennas (2021, 2022, . . . , 202N) respectively to the detection targets 2041, 2042, . . . , 204N, the intensity of the radio waves reflected from the detection targets 2041, 2042, . . . , 204N is calculated.
In the array antenna system disclosed in Patent Document 3, the frequency dependence of the receiving array antennas (2021, 2022, . . . , 202N) is used to control the directivity of the receiving array antennas (2021, 2022, . . . , 202N). In the array antenna system disclosed in Patent Document 3 as well, the intensity of the radio waves reflected from the detection targets 2041, 2042, . . . , 204N is calculated by directing the directivity beam of the receiving array antennas (2021, 2022, . . . , 202N) respectively to the detection targets 2041, 2042, . . . , 204K. The array antenna system disclosed in Patent Document 3 has this point in common with the array antenna systems disclosed in Patent Document 1 and Patent Document 2.
Incidentally, in the array antenna system, because a virtual image of the target 204 is suppressed, there is a constraint that the interval between the respective antennas of the receiving antennas 2021, 2022, . . . , 202N needs to be no more than half the wavelength k of the reflection waves 2031, 2032, . . . , 203N received by the receiver 201.
Patent Document 4 discloses a technique of relaxing the constraint on the interval between the receiving antennas 2021, 2022, . . . , 202N in the array antenna system. In Patent Document 4, a plurality of pulse signals with different RF frequencies are transmitted toward a target, and signals of different RF frequencies reflected from the target are received by a plurality of receiving antennas. The pulse signals of different RF frequencies received by those receiving antennas are phase-aligned and then (coherently) synthesized. By such synthesis processing, a virtual antenna can be formed at a position corresponding to an RF frequency, and as a result, the actual receiving antenna interval can be expanded to at least half of the wavelength λ.
As another system in an imaging device using radio waves, there is a synthetic aperture radar (SAR) system, which is shown in a concept diagram in
The transmitter 311 emits an RF signal (radio wave) 313 from the transmission antenna 312 toward detection targets 3041, 3042, . . . , 304K (where K is the number of targets). The RF signal (radio wave) 313 is reflected at the detection targets 3041, 3042, . . . , 304K, thus respectively generating reflection waves 3031, 3032, . . . , 303K. In this case, the receiver 301, while moving to the position of receivers 3011, 3012, . . . , 301N, receives the reflection waves 3031, 3032, . . . , 303K at the (position of) receiving antennas 3021, 3022, . . . , 302N.
Further, in this case, the receiving antennas 3021, 3022, . . . , 302N, similarly to the receiving antennas 2021, 2022, . . . , 202N in the array antenna system shown in
Therefore, similarly to the array antenna system shown in
Also, examples of a radio wave imaging device using a synthetic aperture radar system are disclosed in Patent Documents 5 to 7.
Here, problems of the array antenna systems (see
The above problem will be specifically explained below. First, in the case of an array antenna system, there is a condition that the respective antenna intervals of the receiving antennas 2021, 2022, . . . , 202N need to be no more than half the wavelength k of the reflection waves 2031, 2032, . . . , 203K received by the receiver 201. In a case where it is not possible to satisfy this condition, there is a problem that a virtual image is generated at a position where the detection targets 2041, 2042, . . . , 204K are not present in a generated image. In a case where the reflection waves 2031, 2032, . . . , 203K are millimeter waves, the wavelength is about several millimeters, and therefore the antenna interval is extremely small.
Next, in the case of an array antenna system, the image resolution is determined by the directivity beam width Δθ of the receiving array antennas (2021, 2022, . . . , 202N). The width Δθ of the directivity beam of the receiving array antennas (2021, 2022, . . . , 202N) is given by Δθ to λ/D. Here, D is the aperture size of the receiving array antennas (2021, 2022, . . . , 202N) and corresponds to the distance between the receiving antenna 2021 and the receiving antenna 202N that are present at both ends. Therefore, in order to obtain a practical resolution in imaging of an article under clothes or an article in a bag, it is necessary to set the aperture size D of the receiving array antennas (2021, 2022, . . . , 202N) to about several tens of cm to several m.
Thus, the array antenna system has two conditions. That is, the respective antenna intervals of the receiving antennas 2021, 2022, . . . , 202N need to be no more than half the wavelength λ (no more than several millimeters), and the distance between the receiving antenna 2021 and the receiving antenna 202N that are present at both ends needs to be at least about several tens of cm. Therefore, if an array antenna system is adopted, then the number N of antennas necessary per row is about several hundred antennas.
Also, an imaging device using actual radio waves needs to form a two-dimensional image. Therefore, as shown in
In this way, an imaging device using a conventional array antenna system requires a large number of antennas and receivers, and therefore the cost is extremely high. Also, since the antennas are spread over an area of several tens of centimeters square to several meters square, the size and weight of the device become very large.
On the other hand, in the array antenna system disclosed in the above-mentioned Patent Document 4, a plurality of pulse signals with different RF frequencies are transmitted and a virtual antenna is formed at a position corresponding to an RF frequency. Thus, suppression of a virtual image is realized while expanding the interval between actual receiving antennas to at least half of the wavelength λ.
However, in the array antenna system disclosed in above Patent Document 4, there is a problem that the range of RF frequencies must be set wide in order to realize high resolution. Specifically, in the array antenna system disclosed in Patent Document 4, when pulse signals of RF frequencies f0, f1, . . . , FN are transmitted, and these are received by two receiving antennas installed with an interval d therebetween, a virtual antenna is installed at a position of d·fn/f0 (where n=0, 1, . . . , N). The effective aperture size D at this time is d·(fN−f0)/f0. From the effective aperture size D, the angular resolution Δθ is given by the following Formula (2).
As can be seen from the above Formula (2), in order to obtain a good angular resolution Δθ, it is necessary to adopt a large RF frequency setting range fN−f0. However, due to the constraint of the radio wave method, it is difficult to adopt a large RF frequency setting range fN−f0, and the value of f0/(fN−f0) is usually about 10 to 100. Here, it is assumed that the receiving antenna interval d in the system of Patent Document 4 is the same as the aperture size D of the array antenna system disclosed in Patent Documents 1 to 3. In this case, the angular resolution in the array antenna system disclosed in Patent Document 4 is f0/(fN−f0) times the angular resolution of the array antenna system disclosed in Patent Documents 1 to 3. In other words, the angular resolution deteriorates by about 10 to 100 times.
Further, in the array antenna system disclosed in Patent Document 4, a pulse signal is used, but in order to obtain distance resolution, it is necessary to set the RF bandwidth of the pulse signal to several hundred MHz to several GHz. In addition, in the pulse radar system adopted in Patent Document 4, the bandwidth of a baseband signal is the same as the RF bandwidth. Therefore, it is necessary for the sampling frequency of the baseband signal to be increased from several hundred MHz to several GHz, which leads to an increase in the amount of calculation. Also, commonly, noise proportional to the bandwidth of the baseband signal is mixed into the baseband signal, but in the pulse radar system, to the extent that the bandwidth of the baseband signal is wide, deterioration of signal quality due to noise is also a problem.
Next, problems of the synthetic aperture radar system disclosed in above Patent Documents 5 to 7 will be described below. A problem with a synthetic aperture radar system is that mechanical movement of the device is required, which makes it difficult to shorten the scanning time. This leads to a problem that the number of targets that can be inspected per unit time is limited when inspecting an article or a person with the imaging device. Also, in particular, the imaging device disclosed in Patent Document 7 requires a mechanical mechanism for moving the receiver, and thus the size and weight of the device increase even more.
As described above, commonly, an imaging device using radio waves has the problem that the cost, size, and weight of the device will be extremely large. On the other hand, if an attempt is made to solve this problem, then the required resolution and signal quality cannot be obtained, and thus a problem of poor accuracy occurs. Therefore, a problem occurs that the applications and opportunities where the imaging device can be actually used are limited. Also, a problem occurs that the speed of inspecting the target is limited.
An example object of the invention is to provide an object detection apparatus, an object detection method, and a computer-readable recording medium that solve the above problems, and whereby, in imaging of an object using radio waves, while suppressing deterioration of image quality, it is possible to reduce the cost and size of the apparatus.
In order to achieve the example object described above, an object detection apparatus according to an example aspect of the invention is an object detection apparatus for detecting an object with radio waves, the object detection apparatus including:
Also, in order to achieve the example object described above, an object detection method according to an example aspect of the invention is a method for detecting an object with radio waves, the object detection method including:
Furthermore, in order to achieve the example object described above, a computer-readable recording medium according to an example aspect of the invention includes,
As described above, according to the invention, in imaging of an object using radio waves, while suppressing deterioration of image quality, it is possible to reduce the cost and size of the apparatus.
Following is a description of example embodiments of a transmission device and a transmission method according to the invention, with reference to the accompanying drawings. In each of the drawings indicated below, the same or corresponding portions are designated by the same reference signs, and a description of such portions is not be repeated.
Below, an object detection apparatus, an object detection method, and a program according to Embodiment 1 of the invention will be described with reference to
[Apparatus Configuration]
First, the configuration of the object detection apparatus according to this Embodiment 1 will be described with reference to
An object detection apparatus 1000 according to this Embodiment 1 shown in
In addition, in the present embodiment, a transmission/reception device 1001 is configured with the transmission unit 1101 and the reception unit 1102, and the object detection apparatus 1000 is mainly configured with the transmission/reception device 1001 and the arithmetic device 1211. Further, the arithmetic device 1211 functions as an arithmetic unit in the object detection apparatus 1000.
The transmission unit 1101 emits a radio wave serving as a transmission signal toward an object that is present on a target arrangement plane 1005 and serves as a detection target (hereinafter referred to as a “target”) 1003.
The reception unit 1102 receives radio waves reflected by the target 1003 as reception signals with a plurality of receiving antennas (see
Specifically, as shown in
The arithmetic device (arithmetic unit) 1211 decides sampling times such that generation of a virtual image due to a beam pattern obtained by synthesizing respective IF signals is suppressed. Further, the arithmetic device 1211 generates an IF signal for detecting the position of the target 1003 (hereinafter referred to as a “position detection IF signal”) by sampling an IF signal at decided sampling times. Then, the arithmetic unit 1211 detects the target 1003 using the position detection IF signal.
Thus, in this Embodiment 1, sampling data obtained by sampling the IF signal at appropriate sampling times can be used as an IF signal from the reception signal received by a virtual antenna. In other words, in this Embodiment 1, a virtual antenna that does not actually exist can be replaced with a receiving antenna in a common array antenna system, and thus it is possible to realize similarly high resolution as a case where a larger number of receiving antennas are provided than the actual number of receiving antennas. Therefore, according to this Embodiment 1, in imaging of an object using radio waves, while suppressing deterioration of image quality, it is possible to reduce the cost and size of the apparatus.
Also, in
Next, the configuration of the object detection apparatus 1000 according to this Embodiment 1 will be described more specifically with reference to
As shown in
In the transmission unit 1101, the oscillator 1201 generates an RF signal (radio wave). The RF signal generated by the oscillator 1201 is transmitted as a transmission signal from the transmission antenna 1202 and emitted to the target 1003. The radio wave reflected by the target 1003 is received by the receiving antenna 1203 in the reception unit 1102.
The mixer 1204 generates an IF signal by mixing the RF signal input from the oscillator 1201 through the terminal 1208 and the radio wave (reception signal) received by the receiving antenna 1203. The IF signal generated by the mixer 1204 is transmitted to the arithmetic device 1211 through the interface circuit 1205. The interface circuit 1205 has a function of converting an IF signal, which is an analog signal, into a digital signal that can be handled by the arithmetic device 1211, and outputs the obtained digital signal to the arithmetic device 1211.
Further, in the example shown in
Specifically, in the example of
In this Embodiment 1, for example, as shown in
Further, in this Embodiment 1, the reception unit 1102 can include a reference receiving antenna and a measurement receiving antenna. In this case, the arithmetic device 1211 executes sampling on an intermediate frequency signal generated from a reception signal received by the measurement receiving antenna and an intermediate frequency signal generated from a reception signal received by the reference receiving antenna.
Then, the arithmetic device 1211, based on obtained sample values, normalizes the IF signal generated from the reception signal received by the measurement receiving antenna according to the IF signal generated from the reception signal received by the reference receiving antenna, and generates a position detection IF signal.
Also, the arithmetic device 1211 can execute processing to limit the position of the target 1003 (the distance to the object detection apparatus 1000) on the IF signal generated from the reception signal received by the measurement receiving antenna and the IF signal generated from the reception signal received by the reference receiving antenna. In this case, the arithmetic device 1211 executes sampling using an IF signal on which processing has been executed.
Further, in the present embodiment, the arithmetic device 1211 calculates a correlation matrix from position detection IF signals, and calculates an evaluation function that represents a position distribution of the target 1003 from the calculated correlation matrix. Also, the arithmetic device 1211 detects the position and shape of the target 1003 using the calculated evaluation function.
Here, a transmission signal emitted to an object in the present embodiment will be described with reference to
In this Embodiment 1, the RF signal generated by the oscillator 1201, as shown in
Also, here, the positional relationship between the target 1003, and the transmission antenna 1202 and the receiving antenna 1203, will be described with reference to
In the example of
As shown in
Also, in the example shown in
[Apparatus Operation]
Next, operation of the object detection apparatus 1000 according to this Embodiment 1 will be described with reference to
As shown in
Next, in the transmission/reception device 1001, the receiving antenna 1203 of the reception unit 1102 receives the radio wave reflected from the target 1003 as a reception signal (step A2).
Next, the reception unit 1102 mixes the respective transmission signals generated by the transmission unit 1101 with the respective reception signals received by each receiving antenna 1203, and generates an IF signal (step A3).
Next, the arithmetic device 1211, based on the respective IF signals obtained from the reception signal of each receiving antenna 1203 in step A3, generates an IF signal such that the distance from the target 1003 to the object detection apparatus 1000 is constrained to a specific value (step A4). Specifically, the arithmetic device 1211 executes processing to limit the detection range of the target 1003 on the IF signal generated from the reception signal received by the measurement receiving antenna and the IF signal generated from the reception signal received by the reference receiving antenna.
Next, the arithmetic device 1211 generates a position detection IF signal using the IF signal of the measurement receiving antenna 1203m (where m=1, 2, . . . , M) and the IF signal of the reference receiving antenna 12030 (Step A5).
Specifically, the arithmetic device 1211 decides sampling times such that generation of a virtual image due to a beam pattern obtained by synthesizing respective IF signals is suppressed. Then, the arithmetic device 1211 performs interpolation processing such that the value of the decided sampling times is obtained, and calculates the value of the IF signal of the measurement receiving antenna 1203m (where m=1, 2, . . . , M) and the value of the IF signal of the reference receiving antenna 12030. Afterward, the arithmetic device 1211 uses the calculated value to normalize the measurement receiving antenna IF signal according to the reference receiving antenna IF signal, and generates a normalized IF signal. This normalized IF signal that is generated is used as the position detection IF signal.
Next, the arithmetic device 1211 calculates an evaluation function from the normalized IF signal, and further calculates the position (distance and angle) of the target 1003 from the evaluation function (step A6).
Next, the arithmetic device 1211 determines whether or not processing has been performed with respect to all predetermined distances (step A7). If the result of the determination in step A7 is Yes, then the arithmetic device 1211 ends operation. On the other hand, if the result of the determination in step A7 is No, then the arithmetic device 1211 executes step A4 again.
Next, steps A3 to A7 among steps A1 to A7 shown in
[Step A3]
First, the details of step A3 will be described, in which the respective transmission signals generated by the transmission unit 1101 are mixed with the reception signals received by each receiving antenna 1203, and an IF signal is generated.
In the arrangement shown in
In the above Formula (3), a represents the chirp rate of the chirp signal shown in
Further, the measurement IF signal (IFm(t)) calculated from the reception signal of the measurement receiving antenna 1203m (where m=1, 2, . . . , M) is given by the following Formula (4). In the following Formula (4), Δdm=dm−d0.
[Step A4]
Next, the details of step A4 will be described, in which the arithmetic device 1211, based on the IF signals obtained from the reception signal of each receiving antenna 1203 in step A3, generates an IF signal such that the distance from the target 1003 to the object detection apparatus 1000 is constrained to a specific value.
In the example shown in
For example, it is assumed that the target 1003 is present at the position of the distance R0 on the target arrangement plane 1005. In this case, the reference IF signal (IF0(t)) of Formula (3) generated by the target 1003 has a frequency of 2αR0/c. Therefore, if Fourier transformation is performed on the time waveform of the reception IF signal obtained by the reference receiving antenna 12030 or the transmission/receiving shared antenna 1210, and only the frequency signal component of 2αR0/c is extracted, an IF signal is obtained such that the position of the target 1003 is constrained to the desired position (distance range).
The measurement IF signal (IFm(t)) in above Formula (4) has a frequency from “2α(R0−Δdm)/c” to “2α(R0+Δdm)/c”. Therefore, if Fourier transformation is performed on the time waveform of the measurement IF signal obtained by the measurement receiving antenna 1203m (where m=1, 2, . . . , M), and only the frequency signal component from 2α(R0−Δdm)/c to 2α(R0+Δdm)/c is extracted, an IF signal is obtained such that the distance value is constrained to R0.
[Step A5]
Next, the details of step A5 will be described, in which the measurement receiving antenna IF signal is normalized according to the reference receiving antenna IF signal, and a normalized IF signal is generated.
As stated in the section describing background art, in an antenna array of a conventional system, in order to prevent the generation of a virtual image, the interval between receiving antennas 202˜ (where n=1, 2, . . . , N) needs to be set to half the wavelength k of the reception wave. Further, in order to realize high resolution, it is necessary to increase the array aperture size (the length from the receiving antenna 2021 to the receiving antenna 202N), and as a result, a large number of receiving antennas 202 are required.
In this Embodiment 1, sampling data of the time waveform of the normalized IF signal rm(t) obtained by dividing the measurement IF signal (IFm(t)) by the reference IF signal (IF0(t)) is used as a virtual antenna array 1301m (where m=1, 2, . . . , M). Then, by using the virtual antenna array 1301m (where m=1, 2, . . . , M) as a substitute for the receiving antennas 202n (where n=1, 2, . . . , N) of the conventional system, high resolution is realized while keeping a small number M of the actual receiving antennas 1203m (where m=1, 2, . . . , M).
In this Embodiment 1, it is necessary to properly set the sampling times of the time waveform and the positions of the actual receiving antennas 1203m (where m=1, 2, . . . , M) in order to prevent the generation of a virtual image. Below, an example of setting the sampling times of the time waveform and the positions of the actual receiving antennas 1203m (where m=1, 2, . . . M) so as to prevent the generation of a virtual image is disclosed.
In step A5, by dividing the measurement IF signal (IFm(t)) by the reference IF signal (IF0(t)), the normalized IF signal rm(t) given by Formula (5) is generated.
The normalized IF signal rm(t) obtained by the receiving antenna 1203m (where m=1, 2, . . . , M) is obtained at sampling times t(m,1), t(m,2), . . . , t(m,p(m)). p(m) is the sampling score of the normalized IF signal obtained by the receiving antenna 1203m. N represents the sum p(1)+p(2)+ . . . +p(M) of the sampling points of all antennas.
A normalized IF signal vector r is defined as follows.
r=[r1,1, . . . ,r1,p(1), . . . ,rM,1, . . . ,rM,p(M)]T,
Here, rm(t(m,n))=rm,n. An Nth-order vector is represented by r. The n-th component rn of the normalized IF signal vector r is expressed by the following Formulas (6) and (7).
The time to in above Formula (7) is the n-th sampling time. The antenna position Δdm changes depending on the value of n.
Next is a description of conditions for generation of a virtual image. When the target 1003 is present in the direction of an angle Go and the conditions of following Formula (8) are satisfied, a virtual image of the target is generated in the direction of an angle G2 where the target 1003 does not originally exist.
[Formula 8]
|Δφn(θn)−Δφn(θ0)|=2π,Δφn(θ)≡φn+1(θ)−φn(θ), (8)
Next, in order to exclude the virtual image, the conditions of following Formula (9) are set.
[Formula 9]
|Δϕn(θa)−Δϕn(θ0)|=2παΔtmΔdm|sin θa−sin θ0|/c≤2π, (9)
In above Formula (9), Δtm represents the sampling cycle of the normalized IF signal rm(t) obtained by the receiving antenna 1203m (where m=1, 2, . . . , M). The condition of the sampling period Δtm where above Formula (9) is satisfied even if the angles θ0 and θa take arbitrary values in the range of −π to +π L is given by the following Formula (10).
As shown in above Formula (10), in this Embodiment 1, it is desirable to set the sampling period Δtm such that if an upper limit is determined according to the position Δdm of the receiving antenna 1203m (where m=1, 2, . . . , M), then the sampling period Δtm will fall within this upper limit.
Also, regarding the receiving antennas 1203m and 1203m+1 adjacent to each other, the conditions of following Formula (11) are set such that the range of phase φn(θ) of above Formula (7) is continuous.
[Formula 11]
fmaxΔdm≥fminΔdm+1,(m=1,2, . . . ,M−1) (11)
In a desirable mode of this Embodiment 1, the antenna position Δdm (where m=1, 2, . . . , M−1) is determined such that the conditions of Formula (11) are satisfied.
When the interval between the receiving antennas 1203m and 1203m+1 adjacent to each other is represented as Δd′m (=Δdm+1−Δdm), above Formula (11) is equivalent to following Formula (12).
That is, in a preferable mode of this Embodiment 1, the interval between the receiving antennas 1203m and 1203m+1 adjacent to each other is set to be no more than an upper limit value determined by the minimum RF frequency fmin and the maximum RF frequency fmax.
In step A5, the arithmetic device 1211 first performs interpolation processing on each of the measurement IF signal (IFm(t)) and the reference IF signal (IF0(t)), and calculates a value for sampling times of the sampling cycle Δtm that satisfies above Formula (10). Next, the arithmetic device 1211 aligns the sampling times of the measurement IF signal (IFm(t)) and the reference IF signal (IF0(t)) by interpolation processing, and then divides the measurement IF signal (IFm(t)) by the reference IF signal (IF0(t)) as indicated in above Formula (5) to calculate the normalized IF signal rm(t) (where m=1, 2, . . . , M).
[Step A6]
Next, the details of step A6 will be described, in which an evaluation function is calculated from a normalized IF signal.
In step A6, the arithmetic device 1211 selects a plurality of ranges of the normalized IF signal, calculates a correlation matrix from the respective plurality of normalized IF signals for which the selected plurality of ranges are prescribed, and then, from an average of the correlation matrix, calculates an evaluation function that represents a position distribution of the target 1003. This point will be described below.
First, in step A6, the arithmetic device 1211 configures a sub-array vector from the normalized IF signal vector r=[r1, r2, . . . , rn, . . . , rN].
Specifically, a v-th sub-array is configured with the reception signal of the v-th to v+W 1-th sub-array, that is, rv=[rv, rv+1, . . . , rv−W+1]T. W corresponds to the number of sampling points included in each sub-array. Therefore, the arithmetic device 1211 calculates a correlation matrix Rcol(v) calculated from the v-th sub-array as shown in following Formula (13). The subscript H in Formula (13) below represents a complex conjugate transposition of the vector.
[Formula 13]
Rcol(v)=rv·rvH, (13)
Rall represents the average of the correlation matrix Rcol(v) (where v=1, 2, . . . , V) of all sub-arrays. The number V of sub-arrays is at least the number K of targets.
In the above method, by utilizing the property that the correlation weakens between the reception signals of different sub-arrays, problems caused by the correlation between reflections can be avoided. Further, in step A6, the arithmetic device 1211 uses a direction vector a(θ) given by the following Formula (14) and the correlation matrix Rall calculated from the normalized IF signal to calculate any of the evaluation functions given by Formulas (15) to (17).
Here, the vector ek (where k=K+1, . . . , W) is a vector whose eigenvalue is equal to noise power among the eigenvectors of the correlation matrix Rall. The phase φ(θ) in Formula (14) is given by the above Formula (7).
The evaluation functions given by Formulas (15) to (17) produce a peak at the angle Ok where the target 1003k (where k=1, 2, . . . , K) is present. Therefore, the arithmetic device 1211 detects the position of the target 1003k from the angle θk at which the peak of the evaluation function of Formulas (15) to (17) is obtained. Furthermore, the arithmetic device 1211 can estimate the distribution of the reflection intensity sk for the target 1003k (where k=1, 2, . . . , K) from the value of the evaluation function.
By the processing up to step A6 above, the distance R0 and the angle θk are determined as an index expressing the position of the target 1003k (where k=1, 2, . . . , K).
[Step A7]
Next is a description of step A7. In steps A1 to A6, a presence angle θk of the target 1003k is calculated after limiting the distance to the specific value R0. Therefore, in step A7, the arithmetic device 1211 determines whether or not processing has been performed with respect to all of the predetermined distances.
If the result of the determination is that processing has not been performed with respect to all distances, the arithmetic device 1211 returns to step A4, changes the limited distance to another value, and then calculates the presence angle θk of the target 1003k. By repeating steps A4 to A7 in this way, the arithmetic device 1211 calculates the presence angle θk of the target 1003k with respect to all of the predetermined distances.
On the other hand, if the result of the determination is that processing has been performed with respect to all distances, then the arithmetic device 1211 completes the processing from step A4 to step A6. Further, when scanning of the distribution of the target 1003k has been completed with all of the predetermined distances and angles, the object detection apparatus 1000 ends this operation.
[Program]
The program according to this Embodiment 1 may be a program that causes a computer to execute steps A1 to A7 shown in
[Apparatus Performance]
Next, the performance of the object detection apparatus 1000 according to the present embodiment, specifically, the resolution of the reflection intensity sk of the target 1003k, will be described.
The resolution of the reflection intensity sk obtained from the evaluation functions of above Formulas (15) to (17) is determined by the beam width formed by the antenna array with the receiving antenna arrangement shown in
In this Embodiment 1, the beam width formed by the antenna array with the receiving antenna arrangement shown in
Further, when the reception signal of the antenna array is given by the above Formula (6), the antenna array directivity (array factor AF(θ)) when the beam is directed in the direction of the angle θ0 is given by the following Formula (18).
Here, u=2πΔq (sin θ−sin θ0). Note that Δq=αΔtmΔdm/c (where m=1, 2, . . . , M). The sampling cycle Δtm corresponding to each receiving antenna is set according to the antenna position Δdm, such that Δq is constant regardless of the antenna number m.
The array factor |AF(θ)| given by the above Formula (18) has its maximum value at the angle θ0, and its peak width, that is, the beam width Δθ, is given by approximately Δθ to 1/NΔq(rad).
That is, the beam width Δθ depends on the sum N of the number of sampling points of all antennas and the parameter Δq determined by the sampling period and the antenna position. Note that the condition of Formula (10), which is a condition that does not allow generation of a virtual image in the range of −π to +π, is a value equivalent to Δq≤½. Δq=½ results in the best beam width (angular resolution) under a condition that does not allow generation of a virtual image in the range of −π to +π, and the beam width (angular resolution) in that case is Δθ to 2/N(rad).
The beam width Δθ, that is, the resolution does not directly depend on the number of antennas M. In other words, this Embodiment 1, in principle, can be configured with only two receiving antennas, namely one reference receiving antenna 12030 and one measurement receiving antenna 12031. Therefore the number of antennas can be significantly reduced in comparison to a conventional method using a large number of antennas. Furthermore, in this Embodiment 1, it is possible to improve the resolution without increasing the number of antennas, by only increasing the total sum N of the number of sampling points.
Also, the beam width Δθ, that is, the resolution does not directly depend on the bandwidth BW of the RF signal. That is, the present embodiment, in principle, can operate even if the bandwidth of the RF signal is set to be arbitrarily narrow. Therefore, this Embodiment 1 can be realized even in a circumstance where the bandwidth of the RF signal that can be used in the radio wave method is constrained. Further, in the present embodiment, it is possible to arbitrarily improve the resolution without expanding the bandwidth BW of the RF signal, by only increasing the total sum N of the number of sampling points.
In this Embodiment 1, use of the FMCW signal is assumed. At this time, the frequency of the IF signal is given by 4BW·R0/cTchip, and in a practical circumstance, the IF frequency is about several tens of kHz to several hundred kHz. In the present embodiment, the sampling rate and the amount of calculation are reduced in comparison to a pulse system in which the bandwidth of the baseband signal is a wide band from several hundred MHz to several GHz, and the problem of signal quality deterioration due to noise is avoided.
As described above, according to the object detection apparatus 1000 and the object detection method in the present embodiment, in comparison to a common array antenna system, the sampling data of the time waveform of the IF signal can be used as a virtual antenna. For this reason, according to this Embodiment 1, a virtual antenna can be substituted for a receiving antenna in a common array antenna system, and therefore high resolution can be realized while reducing the number of receiving antennas.
Also, consider a case compared with a conventional system in which a plurality of pulse signals with different RF frequencies are transmitted and virtual antennas are formed at positions corresponding to the RF frequencies. In a conventional system, it is necessary to set a wide range of RF frequencies in order to realize high resolution, but in this Embodiment 1, sampling data of the time waveform of the IF signal is used as a virtual antenna. Therefore, high resolution operation can be realized even in a circumstance where a wide bandwidth cannot be used for RF signals due to constraints of the radio wave method. Further, in comparison with a conventional system in which pulse signals are used, in this Embodiment 1, the IF signal has a narrow band, so the sampling rate and the amount of calculation are beneficially small, and the problem of signal quality deterioration due to noise can be avoided.
Also, in a conventional synthetic aperture radar system, it is necessary to mechanically move a receiver, and as a result, there is a problem that it takes a long time to detect and inspect an object. On the other hand, in this Embodiment 1, it is sufficient to electronically scan reception frequencies instead of the position of the receiver, so the time needed to detect and inspect an object can be shortened in comparison to a synthetic aperture radar system.
That is, in the object detection apparatus and the object detection method according to this Embodiment 1, the number of required antennas and the number of receivers associated with them can be reduced in comparison to a common array antenna system, so there is the effect that the cost, size, and weight of the apparatus are reduced. Further, in this Embodiment 1, there is the effect that high resolution operation can be realized even in a circumstance where a wide bandwidth cannot be used for RF signals due to constraints of the radio wave method.
Furthermore, in the object detection apparatus and the object detection method according to this Embodiment 1, there is the effect that the sampling rate of the IF signal and the amount of calculation are suppressed to a small amount, so the problem of signal quality deterioration due to noise can be avoided. Also, in the object detection apparatus and the object detection method according to this Embodiment 1, unlike a common synthetic aperture radar system, it is not necessary to mechanically move the apparatus, and as a result, there is the effect that it is possible to shorten the time needed to detect and inspect an object.
Next, an object detection apparatus, an object detection method, and a program according to Embodiment 2 of the invention will be described with reference to
In Embodiment 1 described above, the two-dimensional position of the target 1003 is measured by two variables, namely the distance R0 and the angle θ. On the other hand, in this Embodiment 2, the three-dimensional position of the target 1003 is measured. This will be specifically described below.
[Apparatus Configuration]
The object detection apparatus according to this Embodiment 2 has the same configuration as the object detection apparatus shown in
However, in this Embodiment 2, part of the processing by the arithmetic device 1211 differs from Embodiment 1. Therefore, differences from Embodiment 1 will be described below.
First, the positional relationship between the target 1003, and the transmission/receiving shared antenna 1210 and the receiving antenna 1203, in this Embodiment 2 will be described with reference to
As shown in
As described above, in Embodiment 1, the receiving antenna 1203 is arranged only on the x-axis, whereas in this Embodiment 2, the receiving antenna 1203 is arranged not only on the x-axis but also on the y-axis. This Embodiment 2 differs from Embodiment 1 with respect to the arrangement of the receiving antenna.
Also, in the example of
Next, in the example shown in
[Apparatus Operation]
Next, operation of the object detection apparatus according to this Embodiment 2 will be described. In this Embodiment 2 as well, the object detection method is implemented by operating the object detection apparatus. Therefore, the description of the object detection method in this Embodiment 2 also is replaced with the following description of the operation of the object detection apparatus.
Also, in this Embodiment 2 as well, steps A1 to A7 shown in
[Step A3]
First, the details of step A3 will be described, in which the respective transmission signals generated by the transmission unit 1101 are mixed with the reception signals received by each receiving antenna 1203, and an IF signal is generated.
In the arrangement shown in
The measurement IF signal (IFxm(t)) calculated from the reception signal of the measurement receiving antenna 1203xm (where m=1, 2, . . . , Mx) arranged on the x-axis is given by the following Formula (19).
The measurement IF signal (IFym(t)) calculated from the reception signal of the measurement receiving antenna 1203y, (where m=1, 2, . . . , My) arranged on the y-axis is given by the following Formula (20).
[Step A4]
Next, the details of step A4 will be described, in which the arithmetic device 1211, based on the IF signals obtained from the reception signal of each receiving antenna 1203 in step A3, generates an IF signal such that the distance from the target 1003 to the object detection apparatus is constrained to a specific value.
In the example shown in
For example, it is assumed that the target 1003 is present at the position of the distance R0 on the target arrangement plane 1005. In this case, the reference IF signal (IF0(t)) of Formula (3) generated by the target 1003 has a frequency of 2αR0/c. Therefore, if Fourier transformation is performed on the time waveform of the reception IF signal obtained by the reference receiving antenna 12030 or the transmission/receiving shared antenna 1210, and only the frequency signal component of 2αR0/c is extracted, an IF signal is obtained such that the position of the target 1003 is constrained to the desired position (distance range).
The measurement IF signal (IFxm(t)) in Formula (19) obtained with the receiving antenna 1203xm (where m=1, 2, . . . , Mx) arranged on the x-axis has a frequency from 2α(R0−Δdxm)/c to 2α(R0+Δdxm)/c. Therefore, if Fourier transformation is performed on the time waveform of the measurement IF signal obtained by the measurement receiving antenna 1203m (where m=1, 2, . . . , M), and only the frequency signal component from 2α(R0−Δdxm)/c to 2α(R0+Δdxm)/c is extracted, an IF signal is obtained such that the distance value is constrained to R0.
The same is true for the measurement IF signal (IFym(t)) in Formula (19) obtained with the receiving antenna 1203ym (where m=1, 2, . . . , My) arranged on the y-axis. After Fourier transformation, if only the frequency signal component from 2α(R0−Δdym)/c to 2α(R0+Δdym)/c is extracted, an IF signal constrained to the desired distance range is obtained.
[Step A5]
Next, the details of step A5 will be described, in which the measurement receiving antenna IF signal is normalized according to the reference receiving antenna IF signal, and a normalized IF signal is generated.
In this Embodiment 2, same as in Embodiment 1, the position of the receiving antenna 1203 and the time sampling points are set in accordance with the content disclosed in
Furthermore, in this Embodiment 2, by dividing the measurement IF signal (IFxm(t)) obtained by the measurement receiving antenna 1203xm arranged on the x-axis by the reference IF signal (IF0(t)), a normalized IF signal rxm(t) is generated. The normalized IF signal rxm(t) is given by the following Formula (21).
Similarly, in this Embodiment 2, by dividing the measurement IF signal (IFym(t)) obtained by the measurement receiving antenna 1203ym arranged on the y-axis by the reference IF signal (IF0(t)), a normalized IF signal rym(t) is generated. The normalized IF signal rym(t) is given by the following Formula (22).
The normalized IF signal rxm(t) obtained by the receiving antenna 1203xm (where m=1, 2, . . . , Mx) arranged on the x-axis is acquired at sampling times t(xm,1), t(xm,2), . . . , t(xm,px(m)). The number of sampling points of the normalized IF signal obtained by the receiving antenna 1203xm is represented by px(m). The sum total px(1)+px(2)+ . . . +px(Mx) of the number of sampling points of all antennas is represented by Nx.
Likewise, the normalized IF signal rym(t) obtained by the receiving antenna 1203ym (where m=1, 2, . . . , My) arranged on the y-axis is acquired at sampling times t(ym,1), t(ym,2), . . . , t(ym,py(m)). The number of sampling points of the normalized IF signal obtained by the receiving antenna 1203ym is represented by py(m). The sum total py(1)+py(2)+ . . . +py(My) of the number of sampling points of all antennas is represented by Ny.
A normalized IF signal vector rx related to the receiving antenna 1203xm (where m=1, 2, . . . , Mx) arranged on the x-axis is defined as indicated in the following Formula (23). In Formula (23), rxm(t(m,n))=rxm,n. This vector rx is an Nx-th order vector.
[Formula 23]
rx=[rx1,1, . . . ,rx1,px(1), . . . ,rxM,1, . . . ,rMx,px(Mx)]T, (23)
Likewise, a normalized IF signal vector ry related to the receiving antenna 1203ym (where m=1, 2, . . . , My) arranged on the y-axis is defined as indicated in the following Formula (24). In Formula (24), rym(t(m,n)=rym,n. This vector ry is an Ny-th order vector.
[Formula 24]
ry=[ry1,1, . . . ,ry1,py(1), . . . ,ryM,1, . . . ,rMy,py(My)]T, (24)
Note that in the present embodiment, the sum total Nx of the number of sampling points obtained by the receiving antenna 1203xm (where m=1, 2, . . . , Mx) arranged on the x-axis and the sum total Ny of the number of sampling points obtained by the receiving antenna 1203ym (where m=1, 2, . . . , My) arranged on the y-axis are preferably equal to each other, and in the following description, N=N, =Ny.
The sampling periods of the normalized IF signals rm(t) and rym(t) obtained by the receiving antenna 1203xm and the receiving antenna 1203ym are represented by Δtxm and Δty, respectively. In order to suppress generation of a virtual image, as in Embodiment 1, the conditions indicated in the following Formula (25) are set for the sampling cycle.
Also, the conditions indicated in the following Formulas (26) and (27) are set for the position of receiving antennas such that the phase range is continuous between adjacent receiving antennas, as in Embodiment 1.
[Formula 26]
fmaxΔdxm≤fminΔdx(m+1),(m=1,2 . . . ,Mx−1) (26)
[Formula 27]
fmaxΔdym≥fminΔdy(m+1),(m=1,2, . . . ,My−1) (27)
In step A5, the arithmetic device 1211 first performs interpolation processing on each of the measurement IF signal (IFxm(t)) obtained by the measurement receiving antenna 1203xm arranged on the x-axis and the reference IF signal (IF0(t)). Then, the arithmetic device 1211 calculates a value for sampling times of the sampling cycle Δtxm that satisfies above Formula (25). Next, the arithmetic device 1211 aligns the sampling times of the measurement IF signal (IFxm(t)) and the reference IF signal (IF0(t)) by interpolation processing, and then divides the measurement IF signal (IFm(t)) by the reference IF signal (IF0(t)) as indicated in above Formula (21) to calculate the normalized IF signal rxm(t) (where m=1, 2, . . . , Mx).
Similarly, the arithmetic device 1211 performs interpolation processing on each of the measurement IF signal (IFym(t)) obtained by the measurement receiving antenna 1203ym arranged on the y-axis and the reference IF signal (IF0(t)). Then, the arithmetic device 1211 calculates a value for sampling times of the sampling cycle Δtym that satisfies above Formula (25). Next, the arithmetic device 1211 aligns the sampling times of the measurement IF signal (IFym(t)) and the reference IF signal (IF0(t)) by interpolation processing, and then divides the measurement IF signal (IFym(t)) by the reference IF signal (IF0(t)) as indicated in above Formula (22) to calculate the normalized IF signal rym(t) (where m=1, 2, . . . , My).
[Step A6]
Next, the details of step A6 will be described, in which an evaluation function is calculated from a normalized IF signal.
First, in step A6, the arithmetic device 1211 configures respective sub-array vectors from the normalized IF signal vectors rx=[rx1, rx2, . . . , rx, . . . , rxN]T and ry=[ry1, ry2, . . . , ryn, . . . , ryN]T obtained by the receiving antenna 1203xm arranged on the x-axis and the receiving antenna 1203ym arranged on the y-axis. Specifically, a v-th sub-array is configured with the reception signal of the v-th to v+W−1-th sub-array, that is, rxv=[rxv, rx(v+1), . . . , rx(v+w−1)]T and ryv=[ryv, ry(v+1), . . . , ry(v+w−1)]T. W corresponds to the number of sampling points included in each sub-array.
Next, the arithmetic device 1211 takes the direct product of the sub-array vectors rx, and ryv and generates a normalized IF signal rxyv shown in the following Formula (28).
[Formula 28]
rxyv=rxv⊗ryv=[rxvryv, . . . ,rxvry(v+W−1), . . . ,rx(v+W−1)ryv, . . . ,rx(v+W−1)ry(v+W−1)]T (28)
The normalized IF signal rxyv is a (N2×1)-order vector whose element is the product of all combinations of the elements of rxy and ryv.
Next, the arithmetic device 1211 calculates the correlation matrix Rcol(v) calculated from the v-th sub-array as shown in the following Formula (29).
[Formula 29]
Rcol(v)=rxyv·rxyvH, (29)
Rall represents the average of the correlation matrix Rcol(v) (where v=1, 2, . . . , V) of all sub-arrays. The number V of sub-arrays is at least the number K of targets.
In the above method, by utilizing the property that the correlation weakens between the reception signals of different sub-arrays, problems caused by the correlation between reflections can be avoided.
Next, the arithmetic device 1211 defines a direction vector a(Ox, Oy) given by the following Formula (30).
[Formula 30]
a(θx,θy)=[exp(jφx1,y1), . . . ,exp(jφx1,yW), . . . ,exp(jφxQW,y1), . . . ,exp(jφxW,yW)]T,ϕxn,yn(θx,θy)≡2π(fmin+αtxn)Δdxm sin θx/c+2π(fmin+αtyn)Δdyn sin θy/c, (30)
Also, the times txn and tyn in the above Formula (30) are sampling times corresponding to the n-th component of the normalized IF signal vectors rx and ry, respectively. Further, the antenna positions Δdmx and Δdmy change depending on the value of n.
Next, one of the evaluation functions given by Formulas (31) to (33) is calculated.
The evaluation functions given by Formulas (31) to (33) produce a peak at the angle (θxk, θyk) where the target 1003k (where k=1, 2, . . . , K) is present. Therefore, the arithmetic device 1211 can detect the position of the target 1003k from the angle (θxk, θyk) at which the peak of the evaluation function of Formulas (31) to (33) is obtained. Furthermore, the arithmetic device 1211 can estimate the distribution of the reflection intensity sk for the target 1003k (where k=1, 2, . . . , K) from the value of the evaluation function.
The distance R0 of the target 1003k and the angle (θxk,θyk) are measured in the processing from step A1 to step A6, so the three-dimensional position of the target 1003k can be calculated from that data.
[Step A7]
Next is a description of step A7. In steps A1 to A6, a presence angle (θxk,θyk) of the target 1003k is calculated after limiting the distance to the specific value R0. Therefore, in step A7, the arithmetic device 1211 determines whether or not processing has been performed with respect to all of the predetermined distances.
If the result of the determination is that processing has not been performed with respect to all distances, the arithmetic device 1211 returns to step A4, changes the limited distance to another value, and then calculates the presence angle (θxk, θyk) of the target 1003k. By repeating steps A4 to A7 in this way, the arithmetic device 1211 calculates the presence angle (θxk, θyk) of the target 1003k with respect to all of the predetermined distances.
On the other hand, if the result of the determination is that processing has been performed with respect to all distances, then the arithmetic device 1211 completes the processing from step A4 to step A6. Further, when scanning of the distribution of the target 1003k has been completed with all of the predetermined distances and angles, the object detection apparatus 1000 ends this operation.
[Program]
The program according to this Embodiment 2 may be a program that causes a computer to execute steps A1 to A7 shown in
[Apparatus Performance and Effects in Embodiment 2]
The performance and effects described in Embodiment 1 can be obtained also in this Embodiment 2. Further, according to this Embodiment 2, it is possible to measure the position of the target 1003 in three-dimensional space, so this Embodiment 2 is applicable in more scenes than Embodiment 1.
(Physical Configuration)
Here, a computer (arithmetic device) that realizes an object detection apparatus by executing the program according to Embodiments 1 and 2 will be described with reference to
As shown in
The CPU 111 opens the program (code) according to this example embodiment, which has been stored in the storage device 113, in the main memory 112 and performs various operations by executing the program in a predetermined order. The main memory 112 is typically a volatile storage device such as a DRAM (Dynamic Random Access Memory). Also, the program according to this example embodiment is provided in a state being stored in a computer-readable recording medium 120. Note that the program according to this example embodiment may be distributed on the Internet, which is connected through the communications interface 117.
Also, other than a hard disk drive, a semiconductor storage device such as a flash memory can be given as a specific example of the storage device 113. The input interface 114 mediates data transmission between the CPU 111 and an input device 118, which may be a keyboard or mouse. The display controller 115 is connected to a display device 119, and controls display on the display device 119. Note that the computer 110 may include a GPU (Graphics Processing Unit) or an FPGA (Field-Programmable Gate Array) in addition to the CPU 111 or in place of the CPU 111.
The data reader/writer 116 mediates data transmission between the CPU 111 and the recording medium 120, and executes reading of a program from the recording medium 120 and writing of processing results in the computer 110 to the recording medium 120. The communications interface 117 mediates data transmission between the CPU 111 and other computers.
Also, general-purpose semiconductor storage devices such as CF (Compact Flash (registered trademark)) and SD (Secure Digital), a magnetic recording medium such as a Flexible Disk, or an optical recording medium such as a CD-ROM (Compact Disk Read-Only Memory) can be given as specific examples of the recording medium 120.
Also, instead of a computer in which a program is installed, the object detection apparatus according to this example embodiment can also be realized by using hardware corresponding to each unit. Furthermore, a portion of the object detection apparatus may be realized by a program, and the remaining portion realized by hardware.
Following is a summary of the effects in the present embodiments.
When comparing the common array antenna system described in Patent Documents 1 to 3 with these embodiments, the former array antenna system requires a large number of antennas. On the other hand, in the present embodiments, by using sampling data of the time waveform of IF signals as virtual antennas, and replacing actual receiving antennas with these virtual antennas, high resolution can be realized while reducing the number of receiving antennas.
In the conventional system described in Patent Document 4, in which a plurality of pulse signals with different RF frequencies are transmitted and virtual antennas are formed at positions corresponding to the RF frequencies, it is necessary to set a wide range of RF frequencies in order to realize high resolution. However, in this conventional system, there is a problem that it is difficult to realize high resolution because the range of RF frequencies that can be used in the radio wave method is constrained.
On the other hand, in the present embodiments, by using sampling data of the time waveform of IF signals as virtual antennas instead of forming virtual antennas at positions corresponding to the RF frequencies, it is possible to realize high resolution operation even in a circumstance where a wide bandwidth cannot be used for RF signals due to constraints of the radio wave method.
Further, in the conventional system described in Patent Document 4 based on a pulse system, since the bandwidth of the baseband signal is a wide band from several hundred MHz to several GHz, there are the problems that a high sampling rate and a large amount of calculation are required, and that there is signal quality deterioration due to noise. On the other hand, the present embodiments are based on an FMCW system, so the IF signal bandwidth is a narrow band from several tens of kHz to several hundred kHz, and as a result the sampling rate and the amount of calculation are beneficially small, and the problem of signal quality deterioration due to noise can also be avoided.
When comparing a synthetic aperture radar system with the present embodiments, in a synthetic aperture radar system, it is necessary to mechanically move the receiver 301 (see
That is, in the object detection apparatus and the object detection method according to the present embodiments, the number of required antennas and the number of receivers associated with them can be reduced in comparison to a common array antenna system, so there is the effect that the cost, size, and weight of the apparatus can be reduced. Further, there is the effect that high resolution operation can be realized even in a circumstance where a wide bandwidth cannot be used for RF signals due to constraints of the radio wave method.
Furthermore, there is the effect that the sampling rate of the IF signal and the amount of calculation are suppressed to a small amount, so the problem of signal quality deterioration due to noise can be avoided. Also, in the object detection apparatus and the object detection method according to the present embodiments, unlike a common synthetic aperture radar system, it is not necessary to mechanically move the apparatus, and as a result, there is the effect that it is possible to shorten the time needed to detect and inspect an object.
Some portion or all of the example embodiments described above can be realized according to (supplementary note 1) to (supplementary note 24) described below, but the below description does not limit the invention.
(Supplementary Note 1)
An object detection apparatus for detecting an object with radio waves, the object detection apparatus including:
The object detection apparatus according to supplementary note 1,
The object detection apparatus according to supplementary note 2, wherein the arithmetic unit is configured to:
The object detection apparatus according to supplementary note 2 or 3, wherein the arithmetic unit is configured to;
The object detection apparatus according to supplementary note 4, wherein a plurality of the measurement receiving antennas are provided, and the plurality of measurement receiving antennas are arranged in each of at least two directions with respect to the position of the reference receiving antenna, and the arithmetic unit is configured to:
The object detection apparatus according to any of supplementary notes 1 to 6,
The object detection apparatus according to supplementary note 7,
An object detection method for detecting an object with radio waves, the object detection method including:
The object detection method according to supplementary note 9,
The object detection method according to supplementary note 10,
The object detection method according to supplementary note 10 or 11,
The object detection method according to supplementary note 12,
The object detection method according to supplementary note 12 or 13,
The object detection method according to any of supplementary notes 9 to 14,
The object detection method according to supplementary note 15,
A computer-readable recording medium including,
The computer-readable recording medium according to supplementary note 17,
The computer-readable recording medium according to supplementary note 18,
The computer-readable recording medium according to supplementary note 18 or 19,
The computer-readable recording medium according to supplementary note 20,
The computer-readable recording medium according to supplementary note 20 or 21,
The computer-readable recording medium according to any of supplementary notes 17 to 22,
The computer-readable recording medium according to supplementary note 23,
The configuration of exemplary embodiments of the present invention has been described above. However, the contents disclosed in the above-mentioned patent documents and the like can also be incorporated into the invention by reference. Modifications and adjustments of the exemplary embodiments are possible within the scope of the overall disclosure (including the claims) of the invention and based on the basic technical concepts thereof.
Also, various combinations or selections of various disclosed elements are possible within the scope of the claims of the invention. In other words, the invention of course includes various variations and modifications that can be made by those skilled in the art according to the overall disclosure including the claims and the technical concepts thereof.
Furthermore, the present invention is not limited to the above example embodiments. Within the scope of the present invention, various modifications that can be understood by those skilled in the art can be made to the configuration and details of the present invention.
As described above, according to the invention, in imaging of an object using radio waves, while suppressing deterioration of image quality, it is possible to reduce the cost and size of the apparatus. The present invention is useful in radar devices, imaging devices for inspecting objects under clothes and in bags, and the like.
Filing Document | Filing Date | Country | Kind |
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PCT/JP2018/010755 | 3/19/2018 | WO |
Publishing Document | Publishing Date | Country | Kind |
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WO2019/180767 | 9/26/2019 | WO | A |
Number | Name | Date | Kind |
---|---|---|---|
9035820 | Shiba | May 2015 | B2 |
10788568 | Loui | Sep 2020 | B1 |
20170307729 | Eshraghi | Oct 2017 | A1 |
20170336450 | Cornic et al. | Nov 2017 | A1 |
20180267157 | Guruprasad | Sep 2018 | A1 |
20180348341 | Phelan | Dec 2018 | A1 |
20200300965 | Wu | Sep 2020 | A1 |
Number | Date | Country |
---|---|---|
2000-131409 | May 2000 | JP |
3977751 | Sep 2007 | JP |
4653910 | Mar 2011 | JP |
2011-513721 | Apr 2011 | JP |
5080795 | Nov 2012 | JP |
2013-528788 | Jul 2013 | JP |
2015-14611 | Jan 2015 | JP |
2015-36682 | Feb 2015 | JP |
2015-230216 | Dec 2015 | JP |
2018025421 | Feb 2018 | WO |
Entry |
---|
International Search Report for PCT/JP2018/010755 dated, May 22, 2018 (PCT/ISA/210). |
Written Opinion of the International Searching Authority dated Sep. 22, 2020, in International Application No. PCT/JP2018/010755. |
Number | Date | Country | |
---|---|---|---|
20210033699 A1 | Feb 2021 | US |