METHOD OF DETECTING OBJECT AND APPARATUS THEREFOR

Abstract: An object (5) under-ground (4) is detected by sending an electromagnetic wave pulse from a transmission antenna (2). This is driven by a pulse generator (1) and by detecting the reflectd wave with a receiving antenna (6). The detected wave is divided in the time domain and each divisional waveform is converted into a spectrum in the frequency domain. The evaluation of such parameters as a peak frequency, a DC ratio and a half-power bandwidth enables the discrimination of a certain object of interest, based on the spectrum data. This processing is done by a sampling unit (7) and a computing unit (15) and the sectional image of the detected object is displayed (10).

Description: [Technical Field] This invention relates to a method and apparatus for detecting an invisible object, such as an underground buried object, by transmitting an electromagnetic wave and receiving an echo wave from the object. [Background Art] Fig. 1 is a schematic view showing a measuring system for detecting an underground buried object using an electromagnetic wave. An electric pulse which is sent from pulse generator 1 is fed to transmitting antenna 2 where it is radiated as an electromagnetic wave into the underground. The radiated electromagnetic wave is reflected on an object, such as water layer 17, stone 18, underground buried piping 5, 13, and returned as an echo wave to receiving antenna 6. In a practical measuring apparatus, transmitting and receiving antennas are formed as one system 14. The echo wave is fed via sampling unit 7 to computing unit 9 where it is computed. Then the result of computation is sent to display unit 10. Fig. 2 shows an example of a measurement observation signal which is incident to receiving antenna 6 moved over underground buried piping 5. In Fig. 2, the abscissa represents a time unit which needs to be calculated in terms of the distance. It is, therefore, necessary to compute the velocity of a wave which is propagated across the underground. The velocity is given by: Here, c : velocity of the electromagnetic wave propagated through a free space ε s : relative dielectric constant of the earth. In this connection it is to be noted that it is necessary to measure the relative dielectric constant ε s of the earth at the measuring site. The relative dielectric constant ε s of the earth is generally 4 to 20. The abscissa in the graph of Fig. 2 denotes the round trip time of an electromagnetic wave between the ground surface and the object. In this case, the depth L is expressed as follows: L = T 2 · V (2) where T represents the time of an electromagnetic wave propagated between the ground surface and the object. In actual practice, antenna system 14 including transmitting antenna 2 and receiving antenna 6 is scanned in a direction of arrow 105 of Fig. 1 and an observation signal is stored in computing unit 9 at each time the antenna is moved a distance of 2 cm. At the completion of scanning, the depth is calculated using Equation (2) and observation signals are sequentially arranged in the order in which they are picked up as shown in Fig. 3 (the abscissa: scanning distance; the ordinate: depth of the earth). The amplitude of the observation signal is stepwise distinguished, usually in color, in accordance with the level of the amplitude to form an underground cross-sectional image. Fig. 3 is an example of an underground cross-sectional image as displayed on display unit 10 of Fig. 1. In the graph of Fig. 3, the abscissa denotes the antenna moving distance and the ordinate denotes the depth of the earth, noting that the relative dielectric constant of the earth at a detection site was found to be 16 upon measurement and so calculated and that the observation signal of Fig. 2 corresponds to a dotted line A-A in Fig. 3. In the underground cross-sectional image shown in Fig. 3, a time position for those observation signals of an amplitude of over 30 mV and a time position under 30 mV are indicated by a cross-hatched area and white area, respectively. That is, the amplitude 30 mV is the minimum discrimination amplitude Imin of the observation signal. In order to distinguish the echo waves returned back from the object to be detected, such as the buried piping and water layer, from observation signals, the amplitude magnitudes of the observation signals are employed as a discrimination standard. As shown, for example, in "Applied Science Center for Archaeolog-MASCA Newsletter vol 11 NO2 December 1975, echo wave 11 whose amplitude is greater than a minimum discrimination amplitude Imin as shown in Fig. 2 has been employed as an echo wave returned back from the object, noting that an echo wave 12 denotes a ground surface echo wave. In the case where, for example, there are some objects, such as stone 18, which is distinct from the object to be detected and from which the magnetic wave is strongly returned back, a plurality of echoes 19, 20 appear in the underground cross-section as shown in Fig. 3. This makes it very difficult to distinguish the echo coming from the object, to be detected, from those echoes 19, 20 of objects. A method according to the preamble of claim 1 is known from Chan et.al. "A Characterization of Subsurface Radar Targets", Proceedings of the IEEE, Vol. 67, No. 7, July 1979, pp 991-1000. The document describes the change of an observation signal in the surrounding of an object. All observation signals are subject of FFT processing. The method requires relatively high effort and is not very precise especially in the presence of other reflecting objects. Method and apparatus of the invention are set out in claims 1 and 8, respectively. [Disclosure of Invention] It is accordingly an objective of the present invention to provide an object detection method and apparatus which can positively and accurately detect an object of interest even if there are a plurality of the other object or objects from which an echo wave or waves are returned back. According to the present invention, an object detection method and apparatus are provided which transmit a pulse wave of a broad frequency characteristic into the earth, receive for each scanning distance of an antenna a signal observed as a superimposed echo waves returned back from various objects below the surface of the earth, divide the observation signal into portions for every time interval, convert the divided signal portion into a corresponding frequency region to obtain a spectral distribution, eliminate spurious echo wave from the observation signal with the use of the frequency region data (spectrum peak frequency f p , DC component ratio R dc and half value width W) obtained, and display a result of the elimination processing, as cross-sectional image, on a display unit. Furthermore, the aforementioned method and apparatus perform a correction computation on multi-cross-sectional data obtained as the echo wave and recognize the object of the interest as being an underground buried object of a linear structure. To enhance the horizontal resolution. It is possible to perform a synthetic-aperture-processing on echo waves returned, as a multi-cross-section data, back from an underground buried object of a linear structure and to enhance the amplitude of a signal corresponding to the position of the buried object through the utilization of the horizontal broadening of the electromagnetic wave emitted from the antenna. [Brief Description of the Drawings] Fig. 1 is a block diagram for explaining a conventional object detection method and apparatus; Fig. 2 is a waveform diagram showing an example of one observation signal input to a computing unit in Fig. 1; Fig. 3 shows a cross-sectional image which, when an antenna system is moved in a direction of an arrow in Fig. 1, is constituted from an observation signals; Fig. 4 is a flowchart for explaining the process of detecting an object in accordance with the present invention, as well as the function of an apparatus used for that process, Figs. 4A through Fig. 4D each showing a mode of computation at a different computation stage; Fig. 5 is a graph for explaining an observation signal which is subjected to a waveform analysis, as well as the division of that signal. Fig. 6 shows one of divided signal portions of Fig. 5 and its spectral distribution; Fig. 7 is a graph showing a relation of a DC component ratio of the divided signal portion to a center frequency; Fig. 8 is a graph showing a relation of a half value width of divided signal portions to the center frequency; Fig. 9 is a waveform diagram showing extracted echo wave which is returned back from an object to be detected; Fig. 10 is a cross-sectional image, showing an object, corresponding to the echo wave of Fig. 9; Fig. 11 is a model diagram to explain the measurement of plurality of cross-sectional data; Fig. 12 is a cross-sectional image obtained from the result of processing of multi-cross-section data 1 to n; Fig. 13 is a model diagram for explaining the echo waves, returned back from an object, as being obtained as a hyperbolic configuration; Fig. 14 is a model diagram associated with a synthetic-aperture processing; Fig. 15 is a cross-sectional image, showing an object image, reconstituted by a synthetic-aperture processing; and Fig. 16 is a block diagram for explaining a method and apparatus for detecting an underground buried object in one aspect of the present invention, Figs. 16A to 16D each showing a block diagram of a different internal structure of a computing unit. [Best Mode of Carrying Out the Invention] An explanation will now be given below as to how to detect an underground buried object, such as an underground buried piping, by referring to the accompanying drawings. 1. Method for Detecting an Object The method for detecting an object in accordance with the present invention is characterized in that an object is detected by eliminating spurious echo waves from an observation signal, obtained as various superimposed echo waves from the underground object, with the use of a signal frequency region. The embodiment of the present invention will be explained below in greater detail. Fig. 4 is a flowchart for detecting an object, to be detected, in accordance with the present invention. An explanation of the flowchart of Fig.4 will be given below. Pickup of an Observation Signal A process, up to the picking-up of an observation signal, is based, like the conventional technique of Fig. 1, on the principle of a pulse radar method. First, electric pulses fed from a pulse generator is sent to a transmitting antenna where it is converted into an electromagnetic wave. The electromagnetic wave is radiated into the underground, returned back from an object which is different from the underground area in terms of an electric constant, such as the dielectric constant, and picked up by the receiving antenna. The receiving antenna converts the electromagnetic wave which is returned back from the object into an electric signal which in turn is sampled by a sampling unit to obtain an observation signal as shown, for example, in Fig. 5. By effecting a scanning by moving the transmitting and receiving antennas in one direction, an underground cross-sectional image is obtained which appears along the scanning direction. Stated in more detail, the transmitting and receiving antennas are moved in one direction and an observation signal is collected each time it is moved a distance of 2 cm. The observation signal is converted into depth data on the basis of Equation (2) as set out above and observation signals provide the underground cross-sectional image of which abscissa represents the antenna moving distance and ordinate the depth. Division of an Observation Signal The observation signal appears as superimposed echo waves at underground interfaces, such as layers, stones etc. The echo waves coming from the object being detected are carried, in a time position, on the observation signal. The observation signal is divided into time segments. Two kinds of methods are known; (1) An observation signal is divided by a predetermined time interval ΔT into portions. (2) An observation signal is divided by a zero-crossing method into portions for each time corresponding to one cycle. An observation signal will now be explained as being divided by the zero-crossing method into portions for every time period corresponding to one cycle. Fig. 5 shows an observation signal obtained at step S1 in Fig. 4 and one form of a wave portion divided by the zero-crossing method. The intervals as indicated by an arrow in Fig. 5, each, are a time interval corresponding to one cycle when the zero-crossing method is used and are represented with the waveform number added for each divided wave portion. Here the waveform No. 1 in Fig. 6 at an upper portion is shown as being divided from the observation signal shown in Fig. 5. Conversion into a Frequency Region The divided signal portion is converted into a frequency region by an FFT (Fast Fourier Transformation) in a waveform analytical device so that the spectrum distribution may be found-step S3 (the lower portion in Fig. 6). Reading Out of Features From a spectrum distribution obtained, a strongest peak is found and then the spectrum frequency (spectrum peak frequency) f p , spectrum strength I p for the spectrum frequency f p , DC component strength I dc and half value width W are read out-step S4. Computation of a DC Component Ratio R dc A DC component ratio R dc , that is, a ratio of a DC component strength I dc to a spectrum peak strength I p is computed by the following equation-step S5. R dc = I dc /I p (3) Fig. 6 shows, at the upper portion, a portion divided from the observation signal and, at the lower portion, the spectrum distribution diagram of the divided signal portion with the peak frequency represented by f p and peak strength of the spectrum represented by I p as well as with the DC component strength represented by I dc , and half value width represented by W. Elimination of a Spurious Echo Wave For the divided signal portion of the observation signal the aforementioned processes are repeated at step S3, S4 and S5. For the spectrum peak frequency f p , DC component ratio R dc and half value width W obtained, those divided signal portion having a value range other than f p1 < f p < f p2 , R dc1 < R dc < R dc2 and W₁ < W < W₂ are eliminated as spurious echo waves through the utilization of the characteristics of Figs. 7 and 8. Figs. 7 and 8 are graphs showing f p -R dc and f p -W distributions, respectively, which were obtained from observation signals by various tests conducted. In the graphs shown in Figs. 7 and 8, solids dots represent the characteristic of the echo waves returned back from the underground buried piping and open dots represent the characteristic of the spurious echo waves. From these graphs it has been found that the characteristic of the echo wave returned back from the underground piping is evidently concentrated within a range of f p1 < f p < f p2 , R dc1 < R dc < R dc2 and W₁ < W < W₂. Table 1 shows one example of f p1 , f p2 , R dc1 , R dc2 , W₁ and W₂. f p1 200 (MHz) f p2 300 (MHz) R dc1 0 R dc2 0.1 W₁ 200 (MHz) W₂ 300 (MHz) Some portions are present which satisfy any of the filtering conditions for the center frequency f p , DC component ratio R dc and half value width W. As evident from Table 2, there is only one divided signal portion (wave No. 4) in the observation signal which simultaneously satisfies the aforementioned three conditions. This portion is considered as an echo wave returned back from the underground piping and extracted as such. Here, Table 2 shows the values of the center frequency f p , DC component ratio R dc and half value width W calculated for the divided signal portions in Fig. 5. Echo signal No. f p (MHz) R dc W (MHz) 1 170 0.28 170 2 70 0.8 100 3 170 0.02 200 4 250 0.01 250 5 150 0.25 - 6 70 0.95 120 7 130 0.01 250 8 290 0.02 450 The signal processing (step S6) including the elimination of the spurious echo wave and extraction of the echo wave returned back from the underground piping is performed for an observation signal of Fig. 5. If the aforementioned signal processing is performed for all the observation signals recorded each time the antenna is moved a distance of 2 cm, it is possible to extract only the echo wave returned back from the underground piping. Fig. 10 shows a cross-sectional image reconstituted from observation signals processed by the aforementioned method, noting that the abscissa denotes the antenna scanning distance and the ordinate denotes the depth. The echo wave as shown in Fig. 9 corresponds to a location indicated by the dotted line A-A in Fig. 10. In Fig. 10, a cross-hatched area shows the position where the echo wave of interest is located-step S7. In this way, a specific underground buried object (a steel piping in the present embodiment) can be detected utilizing the characteristics shown in Table 1. Since the boundary condition value of an object (the steel piping in the embodiment), to be detected, is an inherent value, it varies according to type of object being detected. Even if the object being detected is another type of objects, such as a vinyl chloride piping, cavity and earth layer, or some objects in an electromagnetic wave transmission medium, such as steel frames or cracks in the concrete structure, then it is possible to detect the object if the characteristics (f p , R dc , W) of a echo wave returned back from any of these objects is initially found experimentally. The echo wave (returned back from the underground piping) can be extracted by utilizing one characteristic value or a combination of two characteristic values (f p -R dc , f p -W), depending upon the underground state involved. Multi-Cross-Section Processing Although, in the aforementioned embodiment, the computation processing has been explained as the process of extracting the echo wave without considering the length and configuration of the object being detected (step S6a in Fig. 4A), the detection accuracy can be enhanced by performing a correlation computation (step S6b in Fig. 4B) on multi-cross-section data which are picked up in a direction perpendicular to that of the lying of the underground piping, after the echo wave returned back from the object has been extracted (step S6a), in the case where the object is an underground piping of a linear structure. The method for processing the multi-cross-section data will be explained below. The transmitting/receiving antennas are moved in a direction parallel to the antenna scanning line as indicated by an arrow in Fig. 11 to record a plurality of the underground cross-section data. In the case where the object to be detected is underground piping 5 of a linear structure perpendicular to the scanning direction of the antenna, a plurality of cross-section data are subjected to a signal processing to obtain a plurality of cross-sectional images as shown as a measuring cross-section area n for example, in Fig. 12. From the cross-section area thus obtained, echo waves are gained which are present in the same horizontal and vertical positions. The echo waves thus gained are recognized as echo waves returned back from underground piping 5 of a linear structure and the other echo waves are rejected. In this way the correlation computation is performed on the multi-cross-section data to obtain a cross-sectional image as shown previously in Fig. 10. Synthetic-Aperture Processing As shown in Fig. 10, the echo waves returned back from the object take a hyperbolic configuration, because an electromagnetic wave radiated from the antenna is broadened at some angle. This picture is shown in Fig. 13. If the object to be detected and antennas are located in a relative relation as shown in Fig. 13 with L indicating the distance between the antenna and the object, the object is observed in the antenna position X₁ as if it were located at an area a distance L below the antenna. Upon moving the antenna in a direction indicated by the arrow in Fig. 13, the distance L between the antenna and the object becomes small and thus the forward/backward trip T of the electromagnetic wave becomes small. An echo wave obtained when the antenna is located in an area Xo just above the object being detected occupies an apex of the aforementioned hyperbolic configuration. For this reason, in the underground cross-sectional image, a group of echo waves returned back from the object becomes hyperbolic, causing the horizontal resolution to be prominently degraded. In order to enhance the horizontal resolution it is advantageous to perform a synthetic-aperture processing on the underground cross-sectional image which is processed by the aforementioned method. For this reason, subsequent to extracting the echo waves returned back from the object (S6a) in the calculation processing step (Step S6), the synthetic-aperture processing (S6c) is performed as shown in Fig. 4C. Fig. 14 is a principle diagram on which the synthetic-aperture processing is performed. In the diagram shown in Fig. 14, the X- and Z-axes denote the ground surface and depth direction, respectively. In the case where the object to be detected is present at an area (Xo, Zo), the leading edge of the echo wave upon the scanning of the object by the antenna is located on Z = √ (X - Xo)² + Zo² (4) In order to obtain an image of the object at the area (Xo, Zo), therefore, the wave amplitude corresponding to Equation (4) is added to the wave amplitude of the area (Xo, Zo), so that the wave amplitude on the area (Xo, Zo) is grown. In actual practice, since the echo wave is oscillated by an amount ΔL (that is, the echo wavelength ΔL) from the area Zo, the echo wave at the area (Xo, Z) is grown over the range of Z = Zo - Zo + ΔL If the aforementioned processing is performed over a whole coordinates position (X, Z) of the underground cross-sectional image, the maximum amplitude image can be obtained at the area (Xo, Zo) when (X, Z) = (Xo, Zo) Fig. 15 shows an example when the present processing is performed on the underground cross-sectional image of Fig. 10. The horizontal resolution can be enhanced by the present processing on the underground cross-sectional image. Display of a Result of Processing The cross-sectional image, as well as the data processed by the present invention, is output to display unit 10 for display. The synthetic-aperture processing (step S6c) can also be applied to an underground buried piping having a linear structure. In this case, as shown in Fig. 4D, the process (S6a) of extracting echo waves returned back from the object being detected is performed a plurality of times in a direction perpendicular to that in which the piping has been buried, the correlation computation (step S6b) is performed on the multi-cross-section data collected, and finally-the synthetic-aperture processing (step S6c) is performed on the result of correlation computation corresponding to enhance the horizontal resolution. Respective steps S6a, S6b and S6c as shown in Fig. 4D are the same as in Figs. 4A to 4C and further explanation is omitted. 2. Object Detection Apparatus The object detection apparatus according to the embodiment of the present invention will now be explained below. Fig. 16 is a schematic view showing an object detection apparatus according to the embodiment of the present invention which detects an underground buried object. In Fig. 16, pulse generator 1 is adapted to generate an impulse (monopulse) signal having a high output level, transmitting antenna 2 having a broad-band frequency characteristic is adapted to radiate an electromagnetic wave. Reference numerals 3, 4 and 5 show a ground surface, underground area and underground buried piping, respectively. Receiving antenna 6 having a broad-band frequency characteristic is adapted to collect the electromagnetic wave returned back from the object and to convert it into an electric signal. In this connection it is to be noted that, in the present embodiment, the transmitting and receiving antennas, though being shown as separate ones, may be constructed of a single transmitting/receiving antenna. 14 shows an antenna system with transmitting and receiving antennas 2 and 6 mounted thereon. Sampling device 7 is provided for sampling a signal which is sent from receiving antenna 2. Computing unit 15 is provided to divide an observation signal into given time intervals and to perform a fast Fourier transformation for each divided signal portion. Display unit 10 is connected to computing unit 15. The operation of the object detection apparatus of the present invention will now be explained below in more detail. Transmitting and receiving antennas 2 and 6 are set near the ground surface. A high-output electric pulse is sent from pulse generator 1 to transmitting antenna 2 where an electromagnetic wave is radiated into the underground area. The electromagnetic wave propagates into the underground area and is returned, as echo waves, back from various objects having a different electric constant, such as the dielectric constant. The echo wave is picked up by antenna 6 and converted into an electric signal. The converted signal is sampled by sampling device 7 and sent as an observation signal to computing unit 15. Computing unit 15 comprises frequency analyzing section 15a as shown, for example, in Fig. 16A. Frequency analyzing section 15a performs the following processes (a) to (e): (a) First, an observation signal which is an analog signal is converted into a digital signal. The digital observation signal is divided into portions for each time interval. Here a division method is by the zero-crossing method to obtain a one-cycle period. (b) The divided signal portion is converted into a frequency region by the FFT (fast Fourier transformation) processing in frequency analyzing section 15a. Here a power spectrum is found that represents the magnitude of an energy corresponding to each frequency component. (c) From the spectrum distribution obtained, a peak strength is found to compute the spectrum frequency (the peak frequency of the spectrum) f p , DC component ratio R dc -See Equation (3)-and half value width W. (d) Section 15a eliminates the spurious echo waves as set forth in section 1 in conjunction with the detection method. That is, if the values f p , R dc and W computed in the process (c) fall within a range of f p1 < f p < f p2 R dc1 < R dc < R dc2 W₁ < W < W₂ , the divided signal portions are determined as echo waves returned back from the underground buried piping. If, on the other hand, the aforementioned values lies outside the aforementioned range, the echo waves are eliminated as spurious echo waves. (e) The echo wave extracted from observation signal, as well as the cross-sectional image, is output to display unit 10 as shown in Fig. 16. As shown in Fig. 16B, computing unit 15 comprises frequency analyzing section 15a and multi-cross-section correlation processing 15b performing a correlation computation. From the multi-cross-section data subjected to the signal processing, echo waves present in the same horizontal and vertical positions are recognized as echo waves returned back from the buried piping having a linear structure and the other echo waves can be eliminated. Computing unit 15 comprises frequency analyzing section 15a and synthetic aperture processing section 15c as shown in Fig. 16c. Echo waves, which are returned back from the object 5 being detected and obtained by frequency analysis, become hyperbolic. In the case where the buried pipings are located nearby, the hyperbolas are overlapped with respect to each other, prominently degrading the horizontal resolution. Here the amplitude of waves present in the hyperbolic form is additively combined with the amplitude of the wave present at the apex of the hyperbola to obtain a maximum amplitude image at that apex, so that the horizontal resolution can be enhanced. Computing unit 15 comprises frequency analyzing section 15a, multi-cross-section processing section 15b and synthetic-aperture processing section 15c as shown in Fig. 16D. In the case the object to be detected is an underground buried piping having a linear structure, a correlation computation is performed, by multi-cross-section processing section 15b, on a plurality of cross-section data which has been obtained by frequency analyzing section 15a. Then echo waves other than those echo waves returned back from the buried piping are eliminated, and the synthetic-aperture processing is performed by synthetic aperture processing section 15c, on the echo waves. As a result, a cross-sectional image of better horizontal resolution can be obtained with respect to the underground buried piping of a linear structure. If the cross-sectional image of the present application is used as set out above, it is possible to clearly recognize the presence and position of the buried piping. Even if the echo waves returned back from the buried piping cannot be distinguished from the observation signal in a time zone due to the greater attenuation of the electromagnetic wave, it is still possible to achieve a sharp distinction with high accuracy and high resolution when the aforementioned method is employed. Although the present invention has been explained as being applied to the detection of the underground buried object, it is still possible to detect an object of interest below the ground surface even if, echo waves returned back from a target object cannot clearly been distinguished from spurious echo waves from the underground stone, etc., whose spurious echo waves have greater amplitude or even if a plurality of unwanted objects are present near one another. The present invention can be applied to the detecting or searching of a cavity, geologic formation or invisible matter under the surface of the earth or ground, for example, the reinforced iron, or cavity, in the concrete structure, and to the recognizing of a object flying in the free-space as opposed to the underground object.

Claims: A method for detecting an object (5, 13, 17, 18) which comprises the steps of: receiving an observation signal for allowing an electromagnetic wave, which is an echo wave returned from an object, to be taken as a time variation in amplitude; extracting an echo wave returned from an object being detected; and displaying a cross-sectional image of the object from said extracted echo wave, characterized by further comprising the steps of: dividing said observation signal into portions for every predetermined time; converting the divided signal portions into frequency regions to find a spectral distribution; reading from the spectral distribution at least two parameter values of a spectral peak frequency f p , DC component ratio R dc and half value width W; and extracting only the echo wave returned from the object being detected, by eliminating as a spurious echo wave, divided signal portions having a value other than that of the spectral peak frequency f p falling within a predetermined frequency range, that of the DC component ratio R dc falling within a predetermined DC component ratio, or that of half value width W falling within a predetermined half value width. A method according to claim 1, characterized by: receiving, as multi-cross-section data, a plurality of observation signals; for allowing an electromagnetic wave which is an echo wave returned back from an object to be taken as a time variation in amplitude; dividing each of said plurality of observation signals into portions for every predetermined time; converting each of the divided signal portions into a corresponding frequency region to find a spectral distribution; reading from the respective spectral distribution corresponding to each of said plurality of the divided signal portion at least two parameter values of a spectral peak frequency f p , DC component ratio R dc and half value width W; extracting only an echo wave returned back from the object by eliminating, as a spurious echo wave, divided signal portions having a value other than that of said spectral peak frequency f p falling within a predetermined frequency range, that of said DC component ratio R dc falling within a predetermined DC component ratio R dc and that of said half value width W falling within a predetermined range; said echo wave including a plurality of echo wave components which are used as multi-cross-section data; performing a correlation computation on multi-cross-section data corresponding to the extracted echo waves and extracting echo waves returned back from an object of a linear structure, and displaying a result of the correlation computation as a cross-sectional image of the object of a linear structure on a display means. A method according to claim 1, characterized by further comprising the steps of: performing a synthetic-aperture processing by evaluating a hyperbolic configuration whose cross-section data corresponds to an echo wave extracted by said extracting step; and displaying a synthetic-aperture-processed signal as the cross-sectional image whose horizontal resolution is improved. A method according to claim 3, characterized by: receiving, as multi-cross-section data, a plurality of observation signals for allowing an electromagnetic wave which is an echo wave returned back from an object to be taken as a time variation in amplitude; dividing the respective observation signal into portions for every predetermined time; converting the divided signal portion into a corresponding frequency region and evaluating a spectral distribution; reading, from the spectrum distribution corresponding to the respective divided signal portion, at least two spectrum distribution parameter values of a spectrum peak frequency f p , DC component ratio R dc and half value width W; extracting only an echo wave from said object by eliminating, as a spurious echo signal from the respective spectrum distribution parameter values, divided signal portions having a value other than that of said spectrum peak frequency f p falling within a predetermined frequency range, that of said DC component ratio R dc falling within a predetermined DC ratio range and that of said half value width W falling within a predetermined half width value W; said echo waves including a plurality of echo wave components which are used as multi-cross-section data; performing a correlation computation on multi-cross-section data corresponding to said extracted echo wave and extracting echo wave returned back from the object of a linear structure; performing a synthetic-aperture processing including calculating hyperbola with (Xo, Zo) as an apex whose cross-section area corresponds to the echo wave extracted and additively combining a wave amplitude on the calculated/hyperbola with the amplitude of the hyperbola apex (Xo, Zo); and displaying the signal, which is subjected to the correlation computation and synthetic-aperture processing, as the cross-sectional image of said object of a linear structure, whose horizontal resolution is enhanced. The method according to one of claims 1, 2 or 4, characterized by dividing said respective observation signal into portions, by a zero-crossing method, for every time corresponding to one cycle. The method according to one of claims 1, 2 or 4, characterized by reading a spectrum intensity I p and DC component strength I dc in the spectrum peak frequency f p and said DC component ratio R dc is computed from an equation given by: R dc = I dc /I p . The method according to one of claims 1, 2 or 4, characterized by eliminating as a spurious echo wave a divided signal portion having a value other than that of said spectrum peak frequency f p falling within a frequency of f p1 < f p < f p2 , that of said DC component ratio R dc falling within a DC component ratio range of R dc1 < R dc < R dc2 or that of said half value width W falling within a range of W₁ < W < W₂. An apparatus for detecting an object (5, 13, 17, 18), which comprises: transmitting/receiving (14) means for transmitting an electromagnetic wave and receiving as an observation signal an echo wave which is the electromagnetic wave returned from the object; sampling means (7) for sampling the observation signal; and display means (10) for displaying the observation signal and the object image as a reconstituted cross-sectional image, characterized by further comprising: signal dividing means (9) for, after converting the observation signal, which has been sampled, into a digital signal through an A/D conversion, dividing the observation signal into signal portions for every predetermined time; means for converting (9, 15) the divided signal portion into a frequency region and evaluating a spectral distribution; and means for detecting (9, 15) said object on the basis of said spectral distribution. The apparatus according to claim 8, characterized in that said detecting means detects an object on the basis of at least two parameter values of a spectrum peak frequency f p , DC component ratio R dc and half value width W which are evaluated from said spectral distribution. The apparatus according to claim 9, characterized in that said detecting means includes a means for extracting only an echo wave from said object by eliminating as a spurious echo wave, divided signal portions having a value other than that of said spectral peak frequency f p falling within a predetermined range, that of said DC component ratio R dc falling within a predetermined DC component range and that of said half value width W falling within a predetermined half value width range. An apparatus according to claim 8, characterized by said transmitting/receiving means (14) which transmit an electromagnetic wave and receive as multi-cross-section data a plurality of observation signals for allowing an electromagnetic wave which is an echo wave returned back from the object to be taken as a time variation in amplitude; means for sampling (7) said plurality of observation signals; means for reading from each spectral distribution corresponding to the respective divided signal portions at least two parameter values of a spectrum peak frequency f p , DC component ratio R dc and half value width W, for eliminating, as a spurious echo wave, divided signal portions having a value other than that of said spectral peak frequency f p falling within a predetermined frequency range, that of said DC component ratio R dc falling within a predetermined DC component range or that of said half value width W falling within a predetermined half value width, and extracting only an echo wave which is returned back from said object; said echo wave including a plurality of echo wave components which are used as multi-cross-section data; means (15b) for performing a correlation computation on said multi-cross-section data corresponding to the extracted echo wave and for extracting only an echo wave which is returned back from said object of a linear structure; and display means for displaying a result of the correlation computation as the cross-sectional image corresponding to said object of a linear structure. An apparatus according to claim 8, characterized by further comprising synthetic-aperture processing means (15c) comprising means for calculating a hyperbolic configuration with points (Xo, Zo) as an apex whose cross-section data corresponds to the echo wave obtained by the step of extracting only an echo wave from said object and means for additively combining an amplitude of the echo wave on the calculated hyperbola with an amplitude on an apex (Xo, Zo) of a hyperbola; and displaying the synthetic-aperture-processed signal as the cross-sectional image whose horizontal resolution is enhanced. An apparatus according to claim 12, characterized by said transmitting/receiving means (14) which transmit an electromagnetic wave and receive as multi-cross-section data a plurality of observation signals which are an echo wave returned back from said object, to be taken as a time variation in amplitude; sampling means (7) for sampling said plurality of observation signals; means for reading at least two spectrum distribution parameter values of a spectrum peak frequency f p , DC component ratio R dc and half value width W and extracting only an echo wave returned back from said object by eliminating as a spurious echo wave, divided signal portions having a value other than that of said spectrum peak frequency f p falling within a predetermined frequency range, that of said DC component ratio R dc falling within a predetermined DC component ratio or that of said half value width W falling within a predetermined half value width; said echo wave including a plurality of echo wave components which are used as multi-cross-section data; means (15b) for performing a correlation computation on respective multi-cross-section data corresponding to the extracted echo wave and extracting only the echo wave from said object of a linear structure; means for displaying said signal, which is subjected to said correlation computation and synthetic-aperture processing, as a cross-sectional image of said object of a linear structure, whose horizontal resolution is enhanced.

Inventors: ARITA, KISHIO, MASUDA, JUNICHI, MATSUDAIRA, YUZO, NAGAI, EIJI, NAGASHIMA, YUJI, SUDO, YOSHIKAZU
Applicants: NIPPON TELEGRAPH AND TELEPHONE CORPORATION
Application year: 1987
Main classification: G01V3
IPC codes: G01V3, G01S13, G01S7