WO1999018428A1 - Radiographic inspection apparatus - Google Patents
Radiographic inspection apparatus Download PDFInfo
- Publication number
- WO1999018428A1 WO1999018428A1 PCT/JP1997/003547 JP9703547W WO9918428A1 WO 1999018428 A1 WO1999018428 A1 WO 1999018428A1 JP 9703547 W JP9703547 W JP 9703547W WO 9918428 A1 WO9918428 A1 WO 9918428A1
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- WIPO (PCT)
- Prior art keywords
- radiation
- array detector
- collimator
- dimensional array
- detector
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- G—PHYSICS
- G21—NUCLEAR PHYSICS; NUCLEAR ENGINEERING
- G21K—TECHNIQUES FOR HANDLING PARTICLES OR IONISING RADIATION NOT OTHERWISE PROVIDED FOR; IRRADIATION DEVICES; GAMMA RAY OR X-RAY MICROSCOPES
- G21K5/00—Irradiation devices
- G21K5/04—Irradiation devices with beam-forming means
Definitions
- the present invention relates to a radiation inspection apparatus, and more particularly to a technique effective for improving the mobility of the apparatus and reducing the radiation dose of radiation.
- Non-destructive inspection means are required to ensure the reliability of these large structures, and inspection equipment that uses radiation such as high-energy X-rays generated by an electron beam accelerator is practical.
- One non-destructive inspection method using radiation is an X-ray transmission test using X-ray film (hereinafter, X-ray is used as a representative of radiation unless otherwise specified).
- This technique is based on the same principle as medical radiography, in which an X-ray film is placed behind the subject and the subject is irradiated with X-rays. The X-ray film is exposed according to the intensity of the X-ray transmitted through the subject. After the X-ray irradiation is completed, the X-ray film can be developed to obtain a transmitted image.
- Irradiation is required. In this case, it is necessary to install a large shield plate to prevent X-ray leakage to the surrounding area. This method is time-consuming and practical for all equipment installation, inspection, and withdrawal. I can't say.
- the apparatus disclosed in Japanese Patent Application Laid-Open No. 5-302997 uses a high-energy X-ray using an accelerator to form a 200-liter drum with metal chips and concrete inside. It is capable of inspection and has tomography and radiography functions (hereinafter referred to as the first conventional technology).
- the apparatus disclosed in Japanese Patent Application Laid-Open No. 5-253309 is used for treating a patient and obtaining a transmission image for confirming the position of the patient.
- the collimator on the source side is divided.
- a movable collimator is provided.
- the linear detector is moved and the movable collimator limits the irradiation field to the width of the linear detector (hereinafter referred to as the fourth section).
- a high-sensitivity solid-state detector semiconductor detector, scintillation detector, etc.
- an image display and processing device mainly composed of a computer is provided.
- Installation and removal can be performed in a short time.
- the inspection device targeted by the present invention can be configured with two-dimensional and one-dimensional detectors, and uses a collimator on the source side corresponding to each detector to prevent unnecessary radiation irradiation. I do.
- the collimator on the source side is used to prevent X-ray irradiation outside the effective range of the detector.
- a collimator having a conical opening hereinafter referred to as a cone beam collimator
- a collimator having a pyramid-shaped opening hereinafter referred to as a horn beam collimator
- a collimator having a fan-shaped opening hereinafter referred to as a fan beam collimator.
- the one-dimensional detector is scanned to obtain a two-dimensional transmission image, scanning of the detector is performed. It is necessary to move the irradiation position of the fan beam collimator in synchronization with the inspection.
- the problems of the above-described device using the two-dimensional array detector and the device using the one-dimensional array detector are summarized.
- the first issue related to the equipment using the two-dimensional array detector is to reduce the weight of the equipment, especially the weight of the two-dimensional array detector radiation detector, in order to improve mobility.
- the second problem is to provide a simple means for arranging a two-dimensional array detector type radiographic inspection apparatus and to reduce the irradiation dose.
- the third issue related to the equipment using the one-dimensional array detector is to provide a simple means of aligning the one-dimensional array detector type radiological inspection equipment and to reduce the irradiation dose. is there.
- the present invention has been made in view of the above background,
- a first object of the present invention is to provide a two-dimensional array detector type radiographic inspection apparatus, in particular, to provide a radiation inspection apparatus that is lightweight and highly mobile.
- a second object of the present invention is to provide a simple arrangement for separating a radiation generator and a radiation inspection apparatus.
- a third object of the present invention is to provide a radiation inspection apparatus capable of reducing the irradiation dose during alignment work.
- a radiation generator and radiation arranged at a position facing each other across an inspection body.
- the radiation detection device includes a two-dimensional array detector, and includes an optical amplification element on a surface of the array detector facing a radiation incident surface.
- the radiation generation apparatus is located at a position facing the radiation generator with the inspection object interposed therebetween.
- a radiation inspection apparatus comprising a radiation detector using a two-dimensional array detector to be arranged, comprising: an adjustment collimator having one or more pinholes or slits at a radiation outlet of the radiation generator; and the two-dimensional array detection.
- a collimator for imaging that irradiates in accordance with the effective range of the instrument is provided and switched.
- a radiation generator having a beam collimator at a radiation exit, and a one-dimensional array detection device arranged at a position opposed to the inspection object.
- a radiation inspection apparatus comprising a radiation detector using a detector, scanning of the one-dimensional array detector with an adjustment collimator having one or more pinholes or slits at a radiation outlet of the radiation generator is performed.
- the collimator for imaging that performs irradiation corresponding to the effective range included is switched, and the one-dimensional array detector rotates about the central axis of the cone beam. It is desirable to rotate each independently by 90 ° or more.
- a radiation generator including a fan beam collimator at a radiation outlet;
- a radiation inspection apparatus comprising a radiation detection apparatus using a one-dimensional array detector arranged at a position facing the inspection object and having a function of scanning in an array direction of the array detector and in a direction perpendicular to the array detector,
- the fan beam collimator and the one-dimensional array detector rotate about the central axis of the fan beam, and the fan beam collimator moves the irradiation field of the fan beam in synchronization with the scanning of the one-dimensional array detector. It is desirable that the rotation be independently 90 ° or more.
- a radiation generating apparatus having a radiation collimator at a radiation exit.
- a radiation inspection apparatus comprising: a radiation detector that uses a one-dimensional array detector arranged at a position facing an inspection object with the one-dimensional array detector interposed therebetween, and has a function of scanning in the direction perpendicular to the array direction of the array detector.
- the fan beam collimator and one-dimensional array detection And the radiation generator rotates the fan beam around the central axis of the fan beam (desirably rotates independently by 90 ° or more), and the radiation generator synchronizes with the scanning of the one-dimensional array detector. Translate or rotate to move through the irradiation field.
- an optical amplifying element is mounted on a light extraction surface of an array scintillator.
- the optical amplifying element By configuring the optical amplifying element with, for example, an organic multilayer film, the optical amplifying function can be realized with a very slight increase in weight.
- thin film forming techniques such as vapor deposition can be used, and a large number of scintillators can be processed at one time.
- an adjustment collimator having one or more pinholes or slits is attached to the radiation outlet of the radiation generator. Since the irradiation pattern from the adjustment collimator is known, the relative positional relationship between the two can be obtained by comparison with the pattern detected by the two-dimensional detector, and the correction amount required for the alignment is determined from the result. When the alignment work is completed, switch to the collimator for shooting.
- the pinholes in the adjustment collimator provide the reference pattern required for alignment and prevent unnecessary irradiation.
- an adjustment device having one or more pinholes or slits at the radiation outlet of the radiation generator is provided. Attach the collimator. Since the irradiation pattern from the adjustment collimator is known, the relative positional relationship between the two can be obtained by comparison with the two-dimensional detection pattern obtained by scanning the one-dimensional detector. The amount of correction required for is determined. When the alignment work is completed, switch to the collimator for photographing. The adjustment collimator pinholes or slits provide the necessary reference pattern for the alignment and prevent unnecessary illumination.
- the scanning is performed by rotating the one-dimensional array detector about the center axis of the cone beam and moving the slit adjustment collimator 90 ° between the slit direction and the array detector array direction. Determine the amount of correction required for alignment without doing this. For example, first, the slit obtains the horizontal position correction amount from the detection pattern of the one-dimensional array detector with respect to the vertical direction. Next, the slit obtains the position correction amount in the vertical direction from the detection pattern of the one-dimensional array detector with respect to the horizontal. The correction amount necessary for real alignment is determined by these two irradiations.
- the scanning direction is selected according to the shape of the inspection object or the situation of the imaging location.
- the fan beam collimator plays a role similar to that of the slit adjusting collimator described above. Therefore, the one-dimensional array detector is rotated about the center axis of the fan beam, and the direction of the thin and wide fan beam (hereinafter referred to as the fan direction) is shifted 90 ° from the direction of the array of the array detector.
- the fan direction the direction of the thin and wide fan beam
- the fan beam collimator provides the necessary reference pattern for the alignment and prevents unnecessary irradiation during the alignment.
- the scanning direction is selected according to the shape of the inspection object or the situation of the imaging location.
- both the fan-beam collimator and the one-dimensional array detector are independently rotated to obtain the detection pattern of the one-dimensional array detector. This determines the amount of correction required for real alignment.
- the fan beam collimator also provides the necessary reference pattern for the alignment and prevents unnecessary irradiation during the alignment.
- the central axis of the radiation generated from the target and the central axis of the fan beam collimator are made to substantially coincide, and the irradiation field of the fan beam collimator is moved in synchronization with the scanning of the one-dimensional array detector.
- the radiation generated from the target has the property that the intensity is higher at the middle L axis and lower at the periphery. Therefore, when operating only the fan beam collimator, if the fan beam collimator is oriented away from the center axis, the weak part of the radiation will be used. Reduce the resolution slightly.
- the center axis of the radiation generated from the target and the center axis of the fan beam collimator should be almost coincident to move the irradiation field of the fan beam collimator in synchronization with the scanning of the one-dimensional array detector. "io- prevents the resolution from deteriorating in the peripheral area.
- the above operation can be achieved by rotating or translating the entire radiation generating apparatus in synchronization with the one-dimensional array detector. However, this can also be achieved by operating the target and the fan beam collimator in the same way, however, in this case, the electron beam is bent by bending the electron beam traveling direction of the accelerator before the target. They should collide at approximately the same angle at approximately the same location on the get.
- the scanning direction is selected according to the shape of the inspection object or the situation of the imaging location.
- FIG. 1 is a perspective view schematically showing a two-dimensional array detector type radiation detector according to one embodiment of the present invention.
- FIG. 2 is a perspective view showing a radiation inspection apparatus according to one embodiment of the present invention.
- FIG. 3 is a configuration diagram showing a radiation inspection apparatus according to one embodiment of the present invention.
- FIG. 4 is a configuration diagram showing a light amplification section of an array detection element constituting a two-dimensional array detector according to one embodiment of the present invention.
- FIG. 5 is a configuration diagram showing a detection element for an array constituting a two-dimensional array detector according to one embodiment of the present invention.
- FIG. 6 is a configuration diagram showing a method of supplying power to the array detection element according to one embodiment of the present invention.
- FIG. 7 is a configuration diagram showing a detection element for an array constituting a two-dimensional array detector according to one embodiment of the present invention.
- FIG. 8 is a perspective view showing a source-side collimator of one embodiment of the present invention
- FIG. 9 is a contour graph showing a two-dimensional detector output of one embodiment of the present invention.
- FIG. 10 is an explanatory diagram showing a method for correcting the influence of a test object on a two-dimensional detector output according to one embodiment of the present invention.
- FIG. 11 is a configuration diagram showing a scanning mechanism and a rotation mechanism of the one-dimensional detector type inspection apparatus according to one embodiment of the present invention.
- FIG. 12 is a configuration diagram showing a scanning mechanism and a rotation mechanism of the one-dimensional detector type inspection apparatus according to one embodiment of the present invention.
- FIG. 13 is a configuration diagram showing a scanning mechanism of the one-dimensional detector type inspection apparatus according to one embodiment of the present invention.
- FIG. 14 is an explanatory view showing an alignment method in the one-dimensional detector type inspection apparatus according to one embodiment of the present invention.
- FIG. 15 is a graph showing a one-dimensional detector output of one embodiment of the present invention.
- FIG. 16 is an explanatory diagram showing a method for correcting the influence of a test object on a one-dimensional detector output according to one embodiment of the present invention.
- FIG. 1 is a perspective view schematically showing a two-dimensional array detector type radiation detector according to one embodiment of the present invention.
- An electron accelerator is used as the source for inspecting large structures.
- the radiation generated there is very strong and has a large structure. This is an indispensable requirement for inspection of structures.
- the high penetrating power makes it difficult to detect the radiation. Therefore, in this apparatus, the array detecting element 21 uses a deep scintillator 211.
- scintillation Ichita usable may if it has a function of emitting fluorescence by irradiation, N al (T l) crystal, C DW_ ⁇ 4 crystals, Z NW_ ⁇ 4 crystal, B i 4 G e 3 ⁇ 1
- the elements are arranged vertically and horizontally to form a two-dimensional array detector with the required effective range.
- the light from the scintillator 211 is amplified by the optical amplifier element 212 where it exits on the side opposite to the radiation incident direction. Then, the two-dimensional imaging device 3 receives the light from each of the array detection devices 21.
- the optical amplifying element 212 is composed of an organic multilayer film, which will be described later, or a hybrid type element of a light receiving element, an amplifying element, and a light emitting element, thereby enabling weight reduction and cost reduction by mass production.
- FIG. 2 is a perspective view showing a radiation inspection apparatus according to one embodiment of the present invention. Bridges of elevated roads have various sizes and structures. Therefore, considering that it can be used without limiting the shooting target. It is desirable to separate radiation generator 1 and radiation detector 2. Furthermore, since inspections are often performed in a state where both parties cannot see through, alignment means is required in a state where both parties cannot see through.
- FIG. 3 is a configuration diagram showing a radiation inspection apparatus according to one embodiment of the present invention. Align radiation generators and radiation detectors with the imaging target, such as a bridge, in between. High-energy radiation with a strong penetrating power is accelerated by the electron beam accelerator 11 and collided with the target 12, and is emitted based on the principle of bremsstrahlung radiation. Live.
- the radiation (X-rays) generated here has a directivity in front but is widely generated, so the collimator 13 is attached to the tip of the target 12 to limit the irradiation field.
- the irradiation field of the collimator 13 roughly corresponds to the effective range of the detector of the radiation detection device to prevent unnecessary irradiation.
- the collimator is preferably made of a material that efficiently absorbs unnecessary radiation, such as lead and tungsten alloy, but is not particularly limited.
- the radiation generator which includes an electron beam accelerator, a target, and a collimator, performs attitude control such as translation and rotation by a drive unit 14.
- the signal from the one-dimensional or two-dimensional array detector 21 is converted into digital data by a signal processor 22.
- the digital data is calculated by a computer 41 and necessary image processing is performed, and a result such as a transmission image is displayed on a display 42.
- recording and printing are performed by recording means and printing means (not shown) as necessary.
- the radiation detecting section composed of the array detector 21 and the signal processing device 22 controls the attitude such as translation and rotation by the driving device 24.
- FIG. 4 is a configuration diagram showing a light amplification section of an array detection element constituting a two-dimensional array detector according to one embodiment of the present invention.
- the optical amplifier consists of an optical-to-electron converter 215, a carrier transporter 216, an electron-to-optical converter 216, and electrodes 213 on both sides.
- the light from the scintillator 211 enters the photoelectron conversion unit 215 through the electrode 213 directly or by reflection and scattering on the inner surface of the scintillator, and generates electric charge.
- the generated charges move due to the electric field applied between the electrodes, and enter the electron-light converter 216.
- the charge becomes light again, and the light passes through the carrier transporter 217 and exits through the electrode 213.
- FIG. 5 is a configuration diagram showing a detection element for an array constituting a two-dimensional array detector according to one embodiment of the present invention.
- the structure is the same as described in FIG.
- a method for extending the electrode 2 13 to the side surface of the scintillator 2 11 will be described.
- the electrode 2 13 on the scintillator side is formed over any one of the side surfaces adjacent to the surface opposite to the radiation incident surface.
- the photo-to-electron converter 2 14, the electron-to-optical converter 2 15, and the carrier transporter 2 16 are sequentially stacked.
- an insulating layer 214 is formed except for a light exit.
- FIG. 6 is a configuration diagram showing a method of supplying power to the array detection element according to one embodiment of the present invention.
- Power supply leads 218 are attached to both sides of the insulating substrate 219, and insertion holes corresponding to the positions of the array detection elements 21 are provided. As described above, if electrodes are formed on the side surfaces of the scintillator, power can be supplied to the optical amplifier via the leads 218.
- FIG. 7 is a configuration diagram showing a detection element for an array constituting a two-dimensional array detector according to one embodiment of the present invention. The same function can be achieved by combining a plurality of functional elements by hybrid, in addition to realizing the optical amplifier section by the organic multilayer film as shown in FIG.
- the light-receiving element 253 is mounted on one side of the flexible substrate, and the amplifying element 254 and the light-emitting element 255 are mounted using the back side.
- the signal from the light receiving element 25 3 can be connected to the amplifying element 2 54 on the opposite side by using the through hole pattern of the flexible board 25 1. The same applies to the connection between the amplifying element 255 and the light emitting element 255.
- the light receiving element 25 3 is attached to the scintillator 2 11 with an optical adhesive 2 52.
- FIG. 8 is a perspective view showing a source-side collimator according to one embodiment of the present invention. If the positions of the radiation generating device 12 and the radiation detecting device 26 are shifted from each other, the resolution decreases, such as chipping or blurring in the transmitted image. Therefore, an alignment is required before shooting.
- an adjustment collimator 13 1 with one pinhole is installed at the center. When measurement is performed in this state, a pattern that comes out of the pinhole, that is, an output appears only at one point, and by specifying the location, the mutual positional relationship can be easily determined. Based on this, the radiation generator 12 and the radiation detector 26 are aligned.
- the adjustment collimator must have a specific pattern, as described above, even if it has multiple pinholes or one or more slits in addition to one pinhole at the center. good.
- FIG. 9 is a contour graph showing a two-dimensional detector output of one embodiment of the present invention. It is an output image from a two-dimensional detector in the case of the pinhole collimator described above. From this result, the position correction amount of the alignment, for example, ⁇ X and ⁇ are determined. Although not shown, the position is corrected by the attitude control means of one or both of the radiation generator and the radiation detector. After the correction, the measurement may be performed again to confirm that the position correction is performed normally.
- FIG. 10 is an explanatory diagram showing a method for correcting the influence of a test object on a two-dimensional detector output according to one embodiment of the present invention.
- an ideal pattern is not always obtained due to the influence of the inside of the subject on the detector output of the pinhole collimator.
- an internal structure such as a steel frame is almost at the center of the pinhole.
- the pattern is included, ideally, a concentric contour pattern is obtained, and one half of the pattern becomes distorted. This is due to the fact that the distorted side causes the radiation intensity to decrease due to the internal steel frame, and it is impossible to predict in advance unless the internal shape is accurately grasped.
- two or more detector output patterns are acquired, and, for example, by displaying the logarithmic difference between the two, the internal structure of the test object is displayed. The effect on the test results can be corrected.
- FIG. 11 is a configuration diagram showing a one-dimensional detector including a source-side collimator and its periphery of a one-dimensional detector type inspection apparatus according to one embodiment of the present invention.
- the shape of the slit of the collimator 144 on the side of the radiation source 12 is determined in accordance with the shape of the translatable sensitive part of the one-dimensional array detector 27 rotatable by the driving device 28.
- the sensitive part has a structure capable of translating within the array detector 27 (The same applies to Fig. 12, Fig. 13, and Fig. 14.) At this time, the mutual distance between the radiation generator and the radiation inspection device affects the dimensions of the slit. You need to choose.
- the slit shape is made variable and adjusted optimally according to the conditions at the shooting site.
- the operating direction of the detector may not always be the same due to the shape of the test object and surrounding conditions.
- FIG. 12 is a configuration diagram showing a scanning mechanism and a rotation mechanism of the one-dimensional detector type inspection apparatus according to one embodiment of the present invention.
- the central axis of the radiation generated from the target and the central axis of the fan beam collimator 142 are substantially coincident with each other, and the fan beam is synchronized with the one-dimensional array detector 27 scanning.
- the irradiation field of the collimator is moved by the driving device 14 on the source side.
- the radiation generated from the target has the property that the intensity increases toward the center axis and decreases toward the periphery.
- the entire radiation generator is primary.
- the drive device 14 allows the fan beam collimator 14 2 and the drive device 28 to independently rotate the three-dimensional array detector 27 by 90 ° or more with respect to the center of the fan beam. is there.
- FIG. 13 is a configuration diagram showing a scanning mechanism of the one-dimensional detector type inspection apparatus according to one embodiment of the present invention.
- this can also be achieved by operating the target and fan beam collimator 142 in the same way.
- the electron beam must be made to collide with the target at substantially the same angle at approximately the same angle by bending the traveling direction of the electron beam of the accelerator before the target.
- it can be realized by attaching a magnetic field generator 161 that bends an electron beam and a universal joint 162 before the target.
- FIG. 14 is an explanatory view showing an alignment method in the one-dimensional detector type inspection apparatus according to one embodiment of the present invention.
- This section describes the alignment procedure for this device.
- the direction of the fan is set vertically by the rotating mechanism on the side of the collimator 14 (not shown), and the array direction of the one-dimensional array detector is set horizontally by the rotating mechanism 28 on the detector to irradiate radiation. .
- the first detection pattern from the one-dimensional array detector is obtained.
- the position correction amount in the horizontal direction is obtained from this detection pattern.
- the fan direction is set to be horizontal
- the array direction of the one-dimensional array detector is set to be vertical, and radiation is applied to obtain a detection pattern from the second one-dimensional array detector.
- the position correction amount in the horizontal direction is obtained from this detection pattern.
- the correction amount necessary for the alignment is determined by the two irradiations.
- FIG. 15 is a graph showing a one-dimensional detector output of one embodiment of the present invention. is there. This is an output image from a one-dimensional detector in the case of a fan beam collimator. The three peaks correspond to the measurement of the irradiation direction of the fan beam in the three directions of the center and two places on both sides. From this result, the position correction amount of the alignment, for example, ⁇ and ⁇ are determined. Although not shown, the position is corrected by the attitude control means of one or both of the radiation generator and the radiation detector. After correction, measurement may be performed again to confirm that the position correction has been performed normally.
- FIG. 16 is an explanatory diagram showing a method for correcting the influence of a test object on a two-dimensional detector output according to one embodiment of the present invention.
- the three peaks correspond to the measurements in three directions: the center and two places on both sides.
- an ideal pattern cannot always be obtained due to the influence of the inside of the subject in the detector output pattern.
- the optical fiber can be used as a means for transmitting a two-dimensional image.
- the light emission pattern at the entrance can be directly transmitted to the exit. Therefore, a planar scintillator or many scintillators
- the light emission image of the radiation detecting unit in which the chillers are two-dimensionally arranged can be connected to an image sensor such as a two-dimensional CCD camera by using a large number of optical fibers.
- ADVANTAGE OF THE INVENTION According to the 1st characteristic of this invention, it is effective in reducing the weight of a radiation detection apparatus, and can enhance the mobility of a radiation inspection apparatus. Furthermore, by using an organic multi-layer type optical amplifying element, a thin film forming technique such as evaporation can be used, and the cost can be reduced by processing a large number of scintillators at once. According to the second feature of the present invention, simple alignment means can be obtained even when the radiation generator and the radiation inspection apparatus are separated by an adjusting collimator such as a pinhole collimator. Unnecessary irradiation can be prevented by using a pinhole or a slit for the adjustment collimator.
- the third aspect of the present invention in addition to the effect of the above-mentioned second aspect, by taking an image while rotating the one-dimensional array detector, it is possible to adapt to the shape of the inspection object or the situation of the imaging place By selecting the scanning direction, the best transmitted image can be obtained.
- the radiation generator and the radiation inspection apparatus are separated by rotating the fan beam collimator and acquiring the data while keeping the angle substantially perpendicular to the array direction of the one-dimensional array detector. Even simpler means of alignment can be obtained.
- the fan beam collimator can prevent unnecessary irradiation.
- high quality transmission images can be obtained by selecting the scanning direction according to the shape of the inspection object or the situation of the imaging location by taking an image while rotating the one-dimensional array detector. .
- the center axis of the radiation generated from the target and the center of the fan beam collimator are obtained.
- a radiation inspection apparatus including a radiation generation apparatus and a radiation detection apparatus disposed at a position facing each other with an inspection object interposed therebetween
- the radiation detection apparatus when configured by a two-dimensional array detector, the array detection is performed.
- An optical amplification element is provided on the surface of the vessel facing the radiation incidence surface.
- the collimator is switched between alignment work and shooting.
- the radiation detector is composed of a one-dimensional array detector, the collimator and the detector can be rotated independently.
- inspection efficiency is improved.
- the same equipment can inspect structures of various dimensions. With a one-dimensional array detector-type radiation inspection system, structures of various dimensions can be inspected with the same device.
- the scanning direction can be selected according to the structure, a high-quality transmission image can be obtained. In addition, reduce unnecessary radiation exposure.
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Abstract
Description
明 細 書 Specification
放射線検査装置 技術分野 Radiation inspection equipment Technical field
本発明は、 放射線検査装置に係り、 特に装置の機動力の向上および放 射線の漏洩線量の低減に有効な技術に関するものである。 背景技術 The present invention relates to a radiation inspection apparatus, and more particularly to a technique effective for improving the mobility of the apparatus and reducing the radiation dose of radiation. Background art
自動車道路や鉄道などの交通網は地震などの災害を受けても確実に機 能することが災害による被害を最小限に止めることと迅速な復旧に必要 である。 特に、 高架の道路や鉄道は地震による被害を受けやすく、 橋脚 部の信頼性が重要である。 これらの大型構造物の信頼性確保には非破壊 での検査手段が必要であり、 電子線加速器で発生する高エネルギー X線 等の放射線を利用した検査装置が実用的である。 放射線を利用した非破 壊検査方法に、 X線フィルムを使用する X線透過試験がある (以下、 特 に断らない限り X線は放射線の代表として用いている) 。 この手法は、 医療用のレン 卜ゲン撮影と同じ原理であり、 X線フィルムを被検体の背 後に設置し、 被検体に向かって X線を照射する。 X線フィルムには被検 体を透過した X線の強度に対応してフィルムの露光が行われる。 X線の 照射を終了後、 X線フィルムを現像処理することによリ透過像を得るこ とができる。 この方法で大型の構造物を撮影するには、 まず、 透過力の 強い加速器等を使った高エネルギー X線源の使用が必要であるとともに, X線フィルムを感光させるのに数 1 0分の照射が必要である。 この場合, 周辺への X線漏洩の防止から大掛かりな遮蔽板の設置を伴う。 この手法 は装置の据え付け, 検査, 撤収のすべてにおいて手間が掛かり実用的と は言えない。 It is necessary for traffic networks such as motorways and railroads to function reliably even in the event of a disaster such as an earthquake, in order to minimize the damage caused by the disaster and to promptly recover. In particular, elevated roads and railways are easily damaged by earthquakes, and the reliability of the piers is important. Non-destructive inspection means are required to ensure the reliability of these large structures, and inspection equipment that uses radiation such as high-energy X-rays generated by an electron beam accelerator is practical. One non-destructive inspection method using radiation is an X-ray transmission test using X-ray film (hereinafter, X-ray is used as a representative of radiation unless otherwise specified). This technique is based on the same principle as medical radiography, in which an X-ray film is placed behind the subject and the subject is irradiated with X-rays. The X-ray film is exposed according to the intensity of the X-ray transmitted through the subject. After the X-ray irradiation is completed, the X-ray film can be developed to obtain a transmitted image. In order to photograph a large structure using this method, it is necessary to first use a high-energy X-ray source using an accelerator or the like with a strong penetrating power, and it takes several 10 minutes to expose the X-ray film. Irradiation is required. In this case, it is necessary to install a large shield plate to prevent X-ray leakage to the surrounding area. This method is time-consuming and practical for all equipment installation, inspection, and withdrawal. I can't say.
また、 特開平 5— 302997 号公報に示されている装置は、 加速器を使用 した高エネルギーの X線を利用することにより、 内部に金属屑やコンク リー トを充填した 2 0 0 リッ トルドラム缶の検査が可能であり、 断層撮 影およびラジオグラフィ機能を備えている (以下、 第 1 の従来技術とす る) 。 The apparatus disclosed in Japanese Patent Application Laid-Open No. 5-302997 uses a high-energy X-ray using an accelerator to form a 200-liter drum with metal chips and concrete inside. It is capable of inspection and has tomography and radiography functions (hereinafter referred to as the first conventional technology).
さらに、 特開昭 53— 72673 号公報に示されている装置では、 線源側の コリメータに関する記述はないが、 二次元検出器に関する記述がある。 つまり、 二次元の透過像を得る手段として、 残光性を有する面状シンチ レータにイメージ増強手段を備えることにより線量の小さな放射性物体 の二次元分布の検出を可能とする (以下、 第 2の従来技術とする) 。 また、 他の技術として、 特開平 5— 322802 号公報に示されている装置 では、 前述の技術と同様に線源側のコリメータに関する記述はないが、 二次元検出器を使用した装置で、 正確な拡大投影像と断層像を得ること ができる。 また、 二次元 X線検出器の中心の法線延長上に X線焦点の位 置を一致させる技術について開示されている (以下、 第 3の従来技術と する) 。 Further, in the apparatus disclosed in Japanese Patent Application Laid-Open No. 53-72673, there is no description about the collimator on the source side, but there is a description about a two-dimensional detector. In other words, as a means to obtain a two-dimensional transmission image, the two-dimensional distribution of radioactive objects with a small dose can be detected by providing an image intensifying means in a planar scintillator having afterglow. Conventional technology). As another technique, in the apparatus disclosed in Japanese Patent Application Laid-Open No. 5-322802, there is no description about the collimator on the source side as in the above-mentioned technique. It is possible to obtain a magnified projected image and tomographic image. Also, there is disclosed a technique for matching the position of the X-ray focal point on the extension of the center line of the two-dimensional X-ray detector (hereinafter, referred to as a third conventional technique).
また、 特開平 5— 253309 号公報に示されている装置は、 放射線を患者 の治療と患者位置確認用の透過像を得るために使用するものであり、 線 源側のコリメ一タは分割した可動コリメ一タを備えており、 透過像を得 る際には線状検出器を移動するとともに可動コリメ一タによリ照射野を 線状検出器の幅内に制限する (以下、 第 4の従来技術とする) 。 発明の開示 The apparatus disclosed in Japanese Patent Application Laid-Open No. 5-253309 is used for treating a patient and obtaining a transmission image for confirming the position of the patient. The collimator on the source side is divided. A movable collimator is provided. When a transmitted image is obtained, the linear detector is moved and the movable collimator limits the irradiation field to the width of the linear detector (hereinafter referred to as the fourth section). Of the prior art). Disclosure of the invention
大部分の橋梁 · 橋脚が存在する市街地で検査するには、 膨大な数の検 査に必要な装置の機動力、 すなわち軽量化と、 周辺環境への配慮から漏 洩線量の低減が必要である。 さらには、 様々な寸法と形態に対応するた めに、 放射線発生装置と放射線検出装置が分離していることが望ましく、 このために、 放射線発生装置と放射線検出装置のァライメン 卜の簡便な 手段が提供されていることと、 ァライメン卜作業中に照射する放射線を 低減することも撮影中の漏洩線量の低減と同様に必要である。 これらを すべて満足することが実用化を左右する。 For inspections in urban areas where most bridges and piers are located, a huge number of inspections are required. It is necessary to reduce the leakage dose because of the mobility of the equipment required for the inspection, that is, weight reduction and consideration for the surrounding environment. Furthermore, it is desirable that the radiation generator and the radiation detector are separated in order to accommodate various dimensions and forms. For this reason, a simple means of alignment between the radiation generator and the radiation detector is required. It is necessary to reduce the amount of radiation provided during the alignment work, as well as to reduce the amount of leakage during imaging. Satisfying all of these will affect practical application.
ここで、 市街地など現地での検査装置に必要な条件をまとめると、 Here, we summarize the conditions required for local inspection equipment, such as in an urban area,
( 1 ) 透過力の強い X線を発生させるために、 電子線加速器を利用した 高エネルギー X線発生装置を備える、 ( 2 ) 周辺環境への X線の漏洩を 低減するために、 X線発生装置に付属するコリメータを備える、 ( 3 ) 短時間で検査を終えるために、 高感度の固体検出器 (半導体検出器, シ ンチレーシヨン検出器など) と信号処理装置を備える、 (4 ) 検査結果 を短時間で評価するために、 計算機を中心に構成する画像表示および処 理装置を備える、 ( 5 ) 据え付け, 撤収が短時間で行える、 などがある。 本発明が対象とする検査装置は二次元および一次元の検出器を使用し た装置構成が可能であり、 不要な放射線照射を防ぐために、 それぞれの 検出器に応じた線源側のコリメータを使用する。 線源側のコリメータは、 検出器の有効範囲以外への X線照射を防ぐ目的で使用する。 (1) Equipped with a high-energy X-ray generator using an electron beam accelerator to generate X-rays with strong penetration power. (2) X-ray generation to reduce leakage of X-rays to the surrounding environment (3) Equipped with a high-sensitivity solid-state detector (semiconductor detector, scintillation detector, etc.) and a signal processing device to complete the inspection in a short time. In order to evaluate in a short time, an image display and processing device mainly composed of a computer is provided. (5) Installation and removal can be performed in a short time. The inspection device targeted by the present invention can be configured with two-dimensional and one-dimensional detectors, and uses a collimator on the source side corresponding to each detector to prevent unnecessary radiation irradiation. I do. The collimator on the source side is used to prevent X-ray irradiation outside the effective range of the detector.
二次元の検出器を使用した装置では、 円錐型の開口部を持つコリメ一 タ (以下、 コーンビームコリメータと称する) または角錐型の開口部を 持つコリメータ (以下、 ホーンビームコリメ一タと称する) を使用する。 一次元の検出器を使用した装置では、 扇型の開口部を持つコリメ一タ (以下、 ファンビームコリメータと称する) の使用が望ましい。 ただし、 二次元の透過像を得るために一次元検出器を走査するので、 検出器の走 査に同期してフアンビームコリメータの照射位置を移動する必要がある。 ここで、 前述の二次元のアレイ検出器を使用した装置と一次元のァレ ィ検出器を使用した装置について課題をまとめる。 二次元のアレイ検出 器を使用した装置に関連して、 第 1 の課題は、 機動力を向上するために、 装置の軽量化、 特に二次元アレイ検出器型放射線検出装置の軽量化であ る。 また、 第 2の課題は、 二次元アレイ検出器型放射線検査装置のァラ ィメン卜の簡便な手段を提供することと、 照射線量の低減である。 一次 元のアレイ検出器を使用した装置に関連して、 第 3の課題は、 一次元ァ レイ検出器型放射線検査装置のァライメン卜の簡便な手段を提供するこ とと、 照射線量の低減である。 In a device using a two-dimensional detector, a collimator having a conical opening (hereinafter referred to as a cone beam collimator) or a collimator having a pyramid-shaped opening (hereinafter referred to as a horn beam collimator) Use In an apparatus using a one-dimensional detector, it is desirable to use a collimator having a fan-shaped opening (hereinafter referred to as a fan beam collimator). However, since the one-dimensional detector is scanned to obtain a two-dimensional transmission image, scanning of the detector is performed. It is necessary to move the irradiation position of the fan beam collimator in synchronization with the inspection. Here, the problems of the above-described device using the two-dimensional array detector and the device using the one-dimensional array detector are summarized. The first issue related to the equipment using the two-dimensional array detector is to reduce the weight of the equipment, especially the weight of the two-dimensional array detector radiation detector, in order to improve mobility. . The second problem is to provide a simple means for arranging a two-dimensional array detector type radiographic inspection apparatus and to reduce the irradiation dose. The third issue related to the equipment using the one-dimensional array detector is to provide a simple means of aligning the one-dimensional array detector type radiological inspection equipment and to reduce the irradiation dose. is there.
前記の第 1 および第 4の従来技術では、 放射線発生装置と放射線検出 装置が共通の架台に設置されているか、 据え付けて固定して使用するこ とを前提としており、 分離してァライメン卜を実施することは想定して いない。 In the first and fourth prior arts described above, it is premised that the radiation generator and the radiation detector are installed on a common base or installed and fixed, and the alignment is performed separately. It is not expected to do so.
大型構造物、 例えば奥行き 1 メ一トルの橋脚を考え、 1 メー トル角を 装置の有効検査範囲に選ぶとする。 このとき、 放射線源の焦点と二次元 アレイ検出器との距離が 4メー トルでは、 検出器の有効範囲が 2メー ト ル角程度必要になる (詳しくは、 放射線源 · 検査物 · 検出装置の位置関 係により多少異なってくる) 。 前記の第 2の従来技術では、 マイクロチ ヤンネルプレートなどの光増幅器を使用するが、 前述の有効範囲を持た せるには一体で製作することは極めて難しいし、 分割するにしても非常 にコストが掛かる。 また、 前記の第 3の従来技術では、 多数の光フアイ バーを使用するために放射線検出装置の重量が嵩み装置が大きくなると ともに機動力が低下する。 さらに、 個々のシンチレ一タに接続するため に非常にコス卜が掛かる。 現場でのァライメントでは、 検査体を挟んで放射線発生装置と放射線 検査装置の両者が全く見通せない場合があリ、 この状態でもァライメン 卜が行える必要がある。 Consider a large structure, for example a pier with a depth of 1 meter, and choose 1 meter angle as the effective inspection range of the equipment. At this time, if the distance between the focal point of the radiation source and the two-dimensional array detector is 4 meters, the effective range of the detector is required to be about 2 meter angle. It differs slightly depending on the position). In the second prior art, an optical amplifier such as a micro-channel plate is used. However, it is extremely difficult to integrally manufacture the optical amplifier to have the above-mentioned effective range. Hang on. Further, in the third prior art, since a large number of optical fibers are used, the weight of the radiation detection device is increased, and the size of the radiation detection device is increased, and the mobility is reduced. Furthermore, it is very costly to connect to individual scintillators. In an on-site alignment, both the radiation generator and the radiation inspection device may not be able to see through the test object at all, and it is necessary to perform alignment even in this state.
本発明は、 前記の背景に鑑みて成されたものであり、 The present invention has been made in view of the above background,
本発明の第 1の目的は、 二次元アレイ検出器型放射線検査装置におい て、 特に、 放射線検出装置を軽量化し機動力の高い放射線検査装置を提 供することである。 A first object of the present invention is to provide a two-dimensional array detector type radiographic inspection apparatus, in particular, to provide a radiation inspection apparatus that is lightweight and highly mobile.
また、 本発明の第 2の目的は、 放射線発生装置と放射線検査装置を分 離するために、 ァライメン卜の簡便な手段を提供することである。 A second object of the present invention is to provide a simple arrangement for separating a radiation generator and a radiation inspection apparatus.
さらに、 本発明の第 3の目的は、 ァライメン ト作業中の照射線量の低 減を可能とする放射線検査装置を提供することである。 Further, a third object of the present invention is to provide a radiation inspection apparatus capable of reducing the irradiation dose during alignment work.
二次元アレイ検出器型放射線検査装置において、 第 1の目的を達成す るために、 本発明の第 1の特徴によれば、 放射線発生装置と、 検査体を 挟んで対向する位置に配置する放射線検出装置からなる放射線検査装置 において、 前記放射線検出装置が二次元アレイ検出器で構成するととも に前記アレイ検出器の放射線の入射面と対向する面に光増幅素子を備え る。 According to a first aspect of the present invention, in a two-dimensional array detector type radiographic inspection apparatus, according to a first aspect of the present invention, there is provided a radiation generator and radiation arranged at a position facing each other across an inspection body. In a radiation inspection apparatus including a detection device, the radiation detection device includes a two-dimensional array detector, and includes an optical amplification element on a surface of the array detector facing a radiation incident surface.
二次元アレイ検出器型放射線検査装置において、 第 2および第 3の目 的を達成するために、 本発明の第 2の特徴によれば、 放射線発生装置と、 検査体を挟んで対向する位置に配置する二次元アレイ検出器を使用した 放射線検出装置からなる放射線検査装置において、 前記放射線発生装置 の放射線出口に一個以上のピンホール、 または、 スリッ トを備えた調整 用コリメータと前記二次元アレイ検出器の有効範囲に対応した照射を行 う撮影用コリメ一タを備えるとともに切り替える。 According to a second feature of the present invention, in a two-dimensional array detector type radiographic inspection apparatus, in order to achieve the second and third objects, according to a second aspect of the present invention, the radiation generation apparatus is located at a position facing the radiation generator with the inspection object interposed therebetween. A radiation inspection apparatus comprising a radiation detector using a two-dimensional array detector to be arranged, comprising: an adjustment collimator having one or more pinholes or slits at a radiation outlet of the radiation generator; and the two-dimensional array detection. A collimator for imaging that irradiates in accordance with the effective range of the instrument is provided and switched.
一次元アレイ検出器型放射線検査装置において、 第 2および第 3の目 的を達成するために、 本発明の第 3の特徴によれば、 放射線出口にコー ンビ一ムコリメータを備えた放射線発生装置と、 検査体を挟んで対向す る位置に配置する一次元アレイ検出器を使用した放射線検出装置からな る放射線検査装置において、 前記放射線発生装置の放射線出口に一個以 上のピンホール、 または、 スリッ トを備えた調整用コリメータと前記一 次元アレイ検出器の走査を含めた有効範囲に対応した照射を行う撮影用 コリメ一タを切り替える、 さらに、 前記一次元アレイ検出器がコーンビ —ムの中心軸を中心に回転する。 それぞれ独立に 9 0 ° 以上回転するこ とが望ましい。 In the one-dimensional array detector type radiation inspection system, the second and third eyes According to a third aspect of the present invention, there is provided a radiation generator having a beam collimator at a radiation exit, and a one-dimensional array detection device arranged at a position opposed to the inspection object. In a radiation inspection apparatus comprising a radiation detector using a detector, scanning of the one-dimensional array detector with an adjustment collimator having one or more pinholes or slits at a radiation outlet of the radiation generator is performed. The collimator for imaging that performs irradiation corresponding to the effective range included is switched, and the one-dimensional array detector rotates about the central axis of the cone beam. It is desirable to rotate each independently by 90 ° or more.
一次元アレイ検出器型放射線検査装置において、 第 2および第 3の目 的を達成するために、 本発明の第 4の特徴によれば、 放射線出口にファ ンビームコリメータを備えた放射線発生装置と、 検査体を挟んで対向す る位置に配置する一次元アレイ検出器を使用し、 アレイ検出器の配列方 向と該直角方向に走査する機能を備えた放射線検出装置からなる放射線 検査装置において、 前記ファンビームコリメータと、 一次元アレイ検出 器がファンビ一ムの中心軸を中心に回転することと、 前記ファンビーム コリメータが一次元アレイ検出器の走査に同期してファンビームの照射 野を移動する。 回転は、 それぞれ独立に 9 0 ° 以上回転することが望ま しい。 According to a fourth aspect of the present invention, in a one-dimensional array detector-type radiographic inspection apparatus, according to a fourth aspect of the present invention, a radiation generator including a fan beam collimator at a radiation outlet; In a radiation inspection apparatus comprising a radiation detection apparatus using a one-dimensional array detector arranged at a position facing the inspection object and having a function of scanning in an array direction of the array detector and in a direction perpendicular to the array detector, The fan beam collimator and the one-dimensional array detector rotate about the central axis of the fan beam, and the fan beam collimator moves the irradiation field of the fan beam in synchronization with the scanning of the one-dimensional array detector. It is desirable that the rotation be independently 90 ° or more.
一次元アレイ検出器型放射線検査装置において、 第 2および第 3の目 的を達成するために、 本発明の第 5の特徴によれば、 放射線出口にファ ンビ一ムコリメ一タを備えた放射線発生装置と、 検査体を挟んで対向す る位置に配置する一次元アレイ検出器を使用し、 アレイ検出器の配列方 向と該直角方向に走査する機能を備えた放射線検出装置からなる放射線 検査装置において、 前記ファンビームコリメータと、 一次元アレイ検出 器がファンビームの中心軸を中心に回転する (それぞれ独立に 9 0 ° 以 上回転することが望ましい。 ) ことと、 前記放射線発生装置が一次元ァ レイ検出器の走査に同期してファンビームの照射野を移動するために、 平行移動または回転する。 According to a fifth aspect of the present invention, in a one-dimensional array detector type radiographic inspection apparatus, according to a fifth aspect of the present invention, there is provided a radiation generating apparatus having a radiation collimator at a radiation exit. A radiation inspection apparatus comprising: a radiation detector that uses a one-dimensional array detector arranged at a position facing an inspection object with the one-dimensional array detector interposed therebetween, and has a function of scanning in the direction perpendicular to the array direction of the array detector. In one embodiment, the fan beam collimator and one-dimensional array detection And the radiation generator rotates the fan beam around the central axis of the fan beam (desirably rotates independently by 90 ° or more), and the radiation generator synchronizes with the scanning of the one-dimensional array detector. Translate or rotate to move through the irradiation field.
本発明の第 1の特徴によれば、 光増幅素子をァレイ用シンチレ一タの 光取り出し面に取り付ける。 光増幅素子を、 例えば、 有機多層膜で構成 することで、 極めて僅かな重量増加により光増幅機能を実現することが できる。 また、 蒸着等の薄膜形成技術が使用でき、 多数のシンチレータ を一度に処理することが可能になる。 According to a first feature of the present invention, an optical amplifying element is mounted on a light extraction surface of an array scintillator. By configuring the optical amplifying element with, for example, an organic multilayer film, the optical amplifying function can be realized with a very slight increase in weight. In addition, thin film forming techniques such as vapor deposition can be used, and a large number of scintillators can be processed at one time.
本発明の第 2の特徴によれば、 ァライメン 卜を行うとき、 放射線発生 装置の放射線出口に一個以上のピンホール、 または、 スリッ トを備えた 調整用コリメータを取り付ける。 調整用コリメータからの照射パターン は既知であるため、 二次元検出器による検出パターンと比較により両者 の相対的な位置関係を求めることができ、 この結果からァライメントに 必要な補正量を決定する。 ァライメン卜作業が完了すれば撮影用のコリ メータに切り替える。 According to the second feature of the present invention, when performing alignment, an adjustment collimator having one or more pinholes or slits is attached to the radiation outlet of the radiation generator. Since the irradiation pattern from the adjustment collimator is known, the relative positional relationship between the two can be obtained by comparison with the pattern detected by the two-dimensional detector, and the correction amount required for the alignment is determined from the result. When the alignment work is completed, switch to the collimator for shooting.
また、 調整用コリメータのピンホールはァライメン 卜に必要な基準パ ターンを提供するとともに、 不要な照射を防止する。 The pinholes in the adjustment collimator provide the reference pattern required for alignment and prevent unnecessary irradiation.
本発明の第 3の特徴によれば、 前述の第 2の特徴と同様に、 ァライメ ン 卜を行うとき、 放射線発生装置の放射線出口に一個以上のピンホール、 または、 スリッ トを備えた調整用コリメータを取り付ける。 調整用コリ メータからの照射パターンは既知であるため、 一次元検出器を走査して 得る二次元の検出パターンと比較により両者の相対的な位置関係を求め ることができ、 この結果からァライメン卜に必要な補正量を決定する。 ァライメント作業が完了すれば撮影用のコリメータに切り替える。 また、 調整用コリメータのピンホール、 または、 スリッ トは、 ァライ メン トに必要な基準パターンを提供するとともに、 不要な照射を防止す る。 According to the third feature of the present invention, similar to the second feature, when performing alignment, an adjustment device having one or more pinholes or slits at the radiation outlet of the radiation generator is provided. Attach the collimator. Since the irradiation pattern from the adjustment collimator is known, the relative positional relationship between the two can be obtained by comparison with the two-dimensional detection pattern obtained by scanning the one-dimensional detector. The amount of correction required for is determined. When the alignment work is completed, switch to the collimator for photographing. The adjustment collimator pinholes or slits provide the necessary reference pattern for the alignment and prevent unnecessary illumination.
さらに、 一次元アレイ検出器をコーンビームの中心軸を中心に回転さ せ、 スリッ 卜の調整用コリメータをスリツ 卜の方向とアレイ検出器のァ レイの方向を 9 0 ° ずらせることにより走査をせずにァライメン卜に必 要な補正量を決定する。 例えばはじめに、 スリッ トが垂直に対する一次 元アレイ検出器の検出パターンから水平方向の位置補正量を得る。 次に、 スリッ 卜が水平に対する一次元アレイ検出器の検出パターンから垂直方 向の位置補正量を得る。 これら 2回の照射によリアライメン 卜に必要な 補正量を決定する。 Furthermore, the scanning is performed by rotating the one-dimensional array detector about the center axis of the cone beam and moving the slit adjustment collimator 90 ° between the slit direction and the array detector array direction. Determine the amount of correction required for alignment without doing this. For example, first, the slit obtains the horizontal position correction amount from the detection pattern of the one-dimensional array detector with respect to the vertical direction. Next, the slit obtains the position correction amount in the vertical direction from the detection pattern of the one-dimensional array detector with respect to the horizontal. The correction amount necessary for real alignment is determined by these two irradiations.
また、 さらに、 一次元アレイ検出器を回転させた状態で撮影すること によリ検査体の形状あるいは撮影場所の状況に応じた走査方向を選択す る。 Further, by scanning the one-dimensional array detector while rotating, the scanning direction is selected according to the shape of the inspection object or the situation of the imaging location.
本発明の第 4の特徴によれば、 フアンビームコリメータが前述のスリ ッ 卜の調整用コリメータと同様の役割を果たす。 したがって、 一次元ァ レイ検出器をファンビームの中心軸を中心に回転させ、 ファンビームの 薄く広がっている方向 (以下、 ファン方向と称する) とアレイ検出器の アレイの方向を 9 0 ° ずらせることにより走査をせずにァライメン卜に 必要な補正量を決定する。 例えばはじめに、 ファン方向を垂直, 一次元 アレイ検出器のアレイ方向を水平にして放射線を照射して一次元アレイ 検出器からの検出バタ一ンを得る。 この検出バタ一ンから水平方向の位 置補正量を得る。 次に、 ファン方向を水平, 一次元アレイ検出器のァレ ィ方向を垂直にして放射線を照射して一次元アレイ検出器からの検出パ ターンを得る。 この検出パターンから水平方向の位置補正量を得る。 以 上、 2回の照射によりァライメン 卜に必要な補正量を決定する。 According to the fourth aspect of the present invention, the fan beam collimator plays a role similar to that of the slit adjusting collimator described above. Therefore, the one-dimensional array detector is rotated about the center axis of the fan beam, and the direction of the thin and wide fan beam (hereinafter referred to as the fan direction) is shifted 90 ° from the direction of the array of the array detector. This determines the amount of correction required for the alignment without scanning. For example, first, the radiation direction is applied with the fan direction vertical and the array direction of the one-dimensional array detector horizontal, and the detection pattern from the one-dimensional array detector is obtained. The position correction amount in the horizontal direction is obtained from this detection pattern. Next, radiation is emitted with the fan direction horizontal and the array direction of the one-dimensional array detector vertical to obtain the detection pattern from the one-dimensional array detector. A horizontal position correction amount is obtained from this detection pattern. Less than Above, the amount of correction required for the alignment is determined by two irradiations.
また、 ファンビームコリメータはァライメントに必要な基準バタ一ン を提供するとともに、 ァライメン 卜中に不要な照射を防止する。 In addition, the fan beam collimator provides the necessary reference pattern for the alignment and prevents unnecessary irradiation during the alignment.
さらに、 一次元アレイ検出器の走査に同期してファンビームの照射野 を移動することによリ、 撮影に必要な部分にのみ放射線の照射を行うと ともに不要な照射を防止する。 Furthermore, by moving the irradiation field of the fan beam in synchronization with the scanning of the one-dimensional array detector, radiation is irradiated only to a portion required for imaging, and unnecessary irradiation is prevented.
また、 さらに、 一次元アレイ検出器を回転させた状態で撮影すること によリ検査体の形状あるいは撮影場所の状況に応じた走査方向を選択す る。 Further, by scanning the one-dimensional array detector while rotating, the scanning direction is selected according to the shape of the inspection object or the situation of the imaging location.
本発明の第 5の特徴によれば、 前述の第 4の特徴と同様に、 ファンビ —ムコリメ一タと一次元アレイ検出器の両者を独立に回転させて一次元 アレイ検出器の検出パターンを得ることによリアライメン卜に必要な補 正量を決定する。 According to the fifth aspect of the present invention, similarly to the fourth aspect, both the fan-beam collimator and the one-dimensional array detector are independently rotated to obtain the detection pattern of the one-dimensional array detector. This determines the amount of correction required for real alignment.
また、 ファンビームコリメータは、 ァライメン トに必要な基準パター ンを提供するとともに、 ァライメント中に不要な照射を防止する。 The fan beam collimator also provides the necessary reference pattern for the alignment and prevents unnecessary irradiation during the alignment.
さらに、 ターゲッ 卜から発生する放射線の中心軸とファンビームコリ メータの中心軸を概ね一致させ、 一次元アレイ検出器の走査に同期して ファンビームコリメータの照射野を移動する。 ターゲッ 卜から発生する 放射線は中' L、軸ほど強度が強く周辺になるほど強度が弱くなる性質があ る。 したがって、 ファンビームコリメ一タのみを操作する場合は、 中心 軸から離れた方向にファンビームコリメータが向いていると放射線の弱 い部分を利用していることになリ、 撮影結果において周辺部の解像度を 僅かに低下させる。 したがって、 ターゲッ トから発生する放射線の中心 軸とファンビームコリメ一タの中心軸を概ね一致させて一次元アレイ検 出器の走査に同期してファンビームコリメ一タの照射野を移動すること " i o - により、 周辺部での解像度の低下を防止する。 前記の操作は、 放射線発 生装置全体を一次元アレイ検出器に同期して回転、 または、 平行移動す ることにより達成できる。 あるいは、 ターゲッ トとファンビームコリメ ータを同じく操作することでも実現できる。 ただし、 この場合には、 加 速器の電子線の進行方向をターゲッ 卜の手前で曲げる等によリ電子線が タ一ゲッ 卜の概ね同じ場所に概ね同じ角度で衝突するようにしなければ ならない。 Furthermore, the central axis of the radiation generated from the target and the central axis of the fan beam collimator are made to substantially coincide, and the irradiation field of the fan beam collimator is moved in synchronization with the scanning of the one-dimensional array detector. The radiation generated from the target has the property that the intensity is higher at the middle L axis and lower at the periphery. Therefore, when operating only the fan beam collimator, if the fan beam collimator is oriented away from the center axis, the weak part of the radiation will be used. Reduce the resolution slightly. Therefore, the center axis of the radiation generated from the target and the center axis of the fan beam collimator should be almost coincident to move the irradiation field of the fan beam collimator in synchronization with the scanning of the one-dimensional array detector. "io- prevents the resolution from deteriorating in the peripheral area. The above operation can be achieved by rotating or translating the entire radiation generating apparatus in synchronization with the one-dimensional array detector. However, this can also be achieved by operating the target and the fan beam collimator in the same way, however, in this case, the electron beam is bent by bending the electron beam traveling direction of the accelerator before the target. They should collide at approximately the same angle at approximately the same location on the get.
また、 さらに、 一次元アレイ検出器の走査に同期してファンビームの 照射野を移動することにより、 撮影に必要な部分にのみ放射線の照射を 行うとともに不要な照射を防止する。 In addition, by moving the irradiation field of the fan beam in synchronization with the scanning of the one-dimensional array detector, radiation is irradiated only to a portion necessary for imaging and unnecessary irradiation is prevented.
さらに、 加えると、 一次元アレイ検出器を回転させた状態で撮影する ことによリ検査体の形状あるいは撮影場所の状況に応じた走査方向を選 択する。 図面の簡単な説明 In addition, by scanning the one-dimensional array detector while rotating, the scanning direction is selected according to the shape of the inspection object or the situation of the imaging location. BRIEF DESCRIPTION OF THE FIGURES
第 1 図は、 本発明の一実施例の二次元アレイ検出器型放射線検出器の 概略を示す斜視図である。 FIG. 1 is a perspective view schematically showing a two-dimensional array detector type radiation detector according to one embodiment of the present invention.
第 2図は、 本発明の一実施例の放射線検査装置を示す斜視図である。 第 3図は、 本発明の一実施例の放射線検査装置を示す構成図である。 第 4図は、 本発明の一実施例の二次元アレイ検出器を構成するアレイ 用検出素子の光増幅部を示す構成図である。 FIG. 2 is a perspective view showing a radiation inspection apparatus according to one embodiment of the present invention. FIG. 3 is a configuration diagram showing a radiation inspection apparatus according to one embodiment of the present invention. FIG. 4 is a configuration diagram showing a light amplification section of an array detection element constituting a two-dimensional array detector according to one embodiment of the present invention.
第 5図は、 本発明の一実施例の二次元アレイ検出器を構成するアレイ 用検出素子を示す構成図である。 FIG. 5 is a configuration diagram showing a detection element for an array constituting a two-dimensional array detector according to one embodiment of the present invention.
第 6図は、 本発明の一実施例のアレイ用検出素子への給電方法を示す 構成図である。 第 7図は、 本発明の一実施例の二次元アレイ検出器を構成するアレイ 用検出素子を示す構成図である。 FIG. 6 is a configuration diagram showing a method of supplying power to the array detection element according to one embodiment of the present invention. FIG. 7 is a configuration diagram showing a detection element for an array constituting a two-dimensional array detector according to one embodiment of the present invention.
第 8図は、 本発明の一実施例の線源側コリメータを示す斜視図である, 第 9図は、 本発明の一実施例の二次元の検出器出力を示す等高線グラ フである。 FIG. 8 is a perspective view showing a source-side collimator of one embodiment of the present invention, and FIG. 9 is a contour graph showing a two-dimensional detector output of one embodiment of the present invention.
第 1 0図は、 本発明の一実施例の二次元の検出器出力において検査体 の影響を補正する方法を示す説明図である。 FIG. 10 is an explanatory diagram showing a method for correcting the influence of a test object on a two-dimensional detector output according to one embodiment of the present invention.
第 1 1 図は、 本発明の一実施例の一次元検出器型検査装置の走査機構 および回転機構を示すための構成図である。 FIG. 11 is a configuration diagram showing a scanning mechanism and a rotation mechanism of the one-dimensional detector type inspection apparatus according to one embodiment of the present invention.
第 1 2図は、 本発明の一実施例の一次元検出器型検査装置の走査機構 および回転機構を示すための構成図である。 FIG. 12 is a configuration diagram showing a scanning mechanism and a rotation mechanism of the one-dimensional detector type inspection apparatus according to one embodiment of the present invention.
第 1 3図は、 本発明の一実施例の一次元検出器型検査装置の走査機構 を示すための構成図である。 FIG. 13 is a configuration diagram showing a scanning mechanism of the one-dimensional detector type inspection apparatus according to one embodiment of the present invention.
第 1 4図は、 本発明の一実施例の一次元検出器型検査装置におけるァ ライメン 卜方法を示す説明図である。 FIG. 14 is an explanatory view showing an alignment method in the one-dimensional detector type inspection apparatus according to one embodiment of the present invention.
第 1 5図は、 本発明の一実施例の一次元の検出器出力を示すグラフで ある。 FIG. 15 is a graph showing a one-dimensional detector output of one embodiment of the present invention.
第 1 6図は、 本発明の一実施例の一次元の検出器出力において検査体 の影響を補正する方法を示す説明図である。 発明を実施するための最良の形態 FIG. 16 is an explanatory diagram showing a method for correcting the influence of a test object on a one-dimensional detector output according to one embodiment of the present invention. BEST MODE FOR CARRYING OUT THE INVENTION
以下に、 本発明の実施例について図面を参照しながら説明する。 Hereinafter, embodiments of the present invention will be described with reference to the drawings.
第 1 図は、 本発明の一実施例の二次元アレイ検出器型放射線検出器の 概略を示す斜視図である。 大型構造物を検査するために線源には電子線 加速器を使用する。 そこで発生する放射線は非常に透過力が強く大型構 造物の検査に必要欠くべからざる要件である。 しかしながら、 透過力が 強いということは、 その放射線を検出するのも難しくなる。 したがって、 この装置では、 アレイ用検出素子 2 1 は奥行きのあるシンチレ一タ 211 を用いる。 ここで使用できるシンチレ一タは、 放射線によって蛍光を発 する機能を有すればよく、 N a l ( T l )結晶, C dW〇4 結晶, Z nW〇 4 結晶, B i 4 G e 3〇 1 2結晶, 蛍光性物質を添加したプラスチックシンチ レ一タなどがあるが、 特に限定するものでない。 素子を縦横に配列し、 必要な有効範囲を有する二次元アレイ検出器を構成する。 シンチレータ 2 1 1からの光は、 放射線の入射方向と反対側へ出るところで光増幅素 子 2 1 2によって光増幅する。 そして、 個々のアレイ用検出素子 2 1力、 らの光を二次元撮像素子 3で受ける。 光増幅素子 2 1 2は、 後述する有 機多層膜、 または、 受光素子 ' 増幅素子 · 発光素子のハイプリッ ド型素 子で構成することにより軽量化と量産による低コス卜化を可能とする。 第 2図は、 本発明の一実施例の放射線検査装置を示す斜視図である。 高架道路の橋脚といっても様々な寸法と構造がある。 したがって、 撮影 対象を限定せずに使用できることを考えると。 放射線発生装置 1 と放射 線検出装置 2 を分離することが望ましい。 さらには、 両者が見通せない 状態で検査する場合が多いために、 両者が見通せない状態でのァライメ ン卜の手段が必要である。 加えるに、 撮影対象が市街地に存在する場合、 周辺への放射線の漏洩を防止する対策が望まれており、 ァライメン卜中 および撮影中での不要な放射線の照射を防止することが重要である。 第 3図は、 本発明の一実施例の放射線検査装置を示す構成図である。 橋梁などの撮影対象を挟んで放射線発生装置と放射線検出装置をァライ メン 卜する。 透過力の強い高エネルギーの放射線は、 電子線加速器 1 1 で電子を加速しターゲッ 卜 1 2に衝突させると制動輻射の原理により発 生する。 ここで発生する放射線 (X線) は、 前方に指向性があるものの 広く発生するのでコリメ一タ 1 3 をタ一ゲッ 卜 1 2の先に取り付けて照 射野を限定する。 コリメータ 1 3の照射野は、 放射線検出装置の検出器 の有効範囲に概ね対応させ不要な照射を防止する。 コリメータの材質は、 不要な放射線を効率よく吸収するものが良く、 鉛, タングステン合金な どが利用できるが、 特に限定するものでない。 電子線加速器 · タ一ゲッ 卜 · コリメータからなる放射線発生部は、 駆動装置 1 4によって並進 · 回転等の姿勢制御を行う。 FIG. 1 is a perspective view schematically showing a two-dimensional array detector type radiation detector according to one embodiment of the present invention. An electron accelerator is used as the source for inspecting large structures. The radiation generated there is very strong and has a large structure. This is an indispensable requirement for inspection of structures. However, the high penetrating power makes it difficult to detect the radiation. Therefore, in this apparatus, the array detecting element 21 uses a deep scintillator 211. Here scintillation Ichita usable may if it has a function of emitting fluorescence by irradiation, N al (T l) crystal, C DW_〇 4 crystals, Z NW_〇 4 crystal, B i 4 G e 3 〇 1 There are two crystals, plastic scintillator to which a fluorescent substance is added, etc., but there is no particular limitation. The elements are arranged vertically and horizontally to form a two-dimensional array detector with the required effective range. The light from the scintillator 211 is amplified by the optical amplifier element 212 where it exits on the side opposite to the radiation incident direction. Then, the two-dimensional imaging device 3 receives the light from each of the array detection devices 21. The optical amplifying element 212 is composed of an organic multilayer film, which will be described later, or a hybrid type element of a light receiving element, an amplifying element, and a light emitting element, thereby enabling weight reduction and cost reduction by mass production. FIG. 2 is a perspective view showing a radiation inspection apparatus according to one embodiment of the present invention. Bridges of elevated roads have various sizes and structures. Therefore, considering that it can be used without limiting the shooting target. It is desirable to separate radiation generator 1 and radiation detector 2. Furthermore, since inspections are often performed in a state where both parties cannot see through, alignment means is required in a state where both parties cannot see through. In addition, when the imaging target is in an urban area, measures to prevent radiation from leaking to the surrounding area are desired, and it is important to prevent unnecessary radiation during alignment and during imaging. FIG. 3 is a configuration diagram showing a radiation inspection apparatus according to one embodiment of the present invention. Align radiation generators and radiation detectors with the imaging target, such as a bridge, in between. High-energy radiation with a strong penetrating power is accelerated by the electron beam accelerator 11 and collided with the target 12, and is emitted based on the principle of bremsstrahlung radiation. Live. The radiation (X-rays) generated here has a directivity in front but is widely generated, so the collimator 13 is attached to the tip of the target 12 to limit the irradiation field. The irradiation field of the collimator 13 roughly corresponds to the effective range of the detector of the radiation detection device to prevent unnecessary irradiation. The collimator is preferably made of a material that efficiently absorbs unnecessary radiation, such as lead and tungsten alloy, but is not particularly limited. The radiation generator, which includes an electron beam accelerator, a target, and a collimator, performs attitude control such as translation and rotation by a drive unit 14.
一次元または二次元のアレイ検出器 2 1 からの信号は、 信号処理装置 2 2によってデジタルデータに変換する。 デジタルデータを計算機 4 1 で演算および必要な画像処理を行い、 透過画像等の結果をディスプレー 4 2に表示する。 また、 必要に応じて図示していない記録手段や印刷手 段によって記録と印刷をする。 アレイ検出器 2 1 と信号処理装置 2 2か らなる放射線検出部は、 駆動装置 2 4によって並進 · 回転等の姿勢制御 を行う。 The signal from the one-dimensional or two-dimensional array detector 21 is converted into digital data by a signal processor 22. The digital data is calculated by a computer 41 and necessary image processing is performed, and a result such as a transmission image is displayed on a display 42. In addition, recording and printing are performed by recording means and printing means (not shown) as necessary. The radiation detecting section composed of the array detector 21 and the signal processing device 22 controls the attitude such as translation and rotation by the driving device 24.
第 4図は、 本発明の一実施例の二次元アレイ検出器を構成するアレイ 用検出素子の光増幅部を示す構成図である。 光増幅部は、 光一電子変換 部 2 1 5, キヤリャ輸送部 2 1 6, 電子一光変換部 2 1 7, 両側の電極 2 1 3で構成する。 シンチレ一タ 2 1 1からの光は、 直接あるいはシン チレ一タの内面での反射と散乱により、 電極 2 1 3 を通して光一電子変 換部 2 1 5へ入り、 電荷を発生する。 発生した電荷は、 電極間に印加す る電界によって移動し、 電子—光変換部 2 1 6へ入る。 ここで、 電荷は 再び光になり、 光はキヤリャ輸送部 2 1 7 を通過して、 電極 2 1 3 を通 つて出る。 ここで、 全体として光増幅を行うには、 光—電子変換部か電 子一光変換部のいずれかまたは両方の層において増幅機能を備えること が必要である。 そのような機能を備えたものに、 例えば、 応用物理学会 誌, 第 6 4巻, 第 1 0号( 1 9 9 5 ) の p . l 0 3 6— 1 0 3 9に述べら れているものが使用できる。 この論文では、 光—電子変換部 2 1 5 とし て、 光電導性ペリ レン顔料, ナフタ レン誘導体, フタロシアニン顔料を 用い、 電子—光変換部 2 1 6 として、 t 一 B u P h— P T C, A 1 q3 を用いている。 FIG. 4 is a configuration diagram showing a light amplification section of an array detection element constituting a two-dimensional array detector according to one embodiment of the present invention. The optical amplifier consists of an optical-to-electron converter 215, a carrier transporter 216, an electron-to-optical converter 216, and electrodes 213 on both sides. The light from the scintillator 211 enters the photoelectron conversion unit 215 through the electrode 213 directly or by reflection and scattering on the inner surface of the scintillator, and generates electric charge. The generated charges move due to the electric field applied between the electrodes, and enter the electron-light converter 216. Here, the charge becomes light again, and the light passes through the carrier transporter 217 and exits through the electrode 213. Here, in order to perform optical amplification as a whole, it is necessary to provide an amplification function in one or both layers of the photo-electron converter and the electronic-optical converter. is necessary. Such a function is described, for example, in the Journal of the Japan Society of Applied Physics, Vol. 64, No. 10 (1995), p. Things can be used. In this paper, we used a photoconductive perylene pigment, a naphthalene derivative, and a phthalocyanine pigment as the photo-electron conversion unit 215, and used t-Bu Ph-PTC as the electron-light conversion unit 216. A 1 q 3 is used.
全体として、 さらに、 光一光増幅率を上げるには、 図示しないが、 前 述の光増幅層を複数回積層することにより可能である。 As a whole, to further increase the light-to-light amplification factor, it is possible to stack the above-described light amplification layers a plurality of times, although not shown.
第 5図は、 本発明の一実施例の二次元アレイ検出器を構成するアレイ 用検出素子を示す構成図である。 構造は第 4図で述べたものと同じであ る。 ここでは、 電極 2 1 3 をシンチレ一タ 2 1 1の側面に延長する方法 について示す。 例えば、 シンチレ一タ側の電極 2 1 3 を放射線の入射面 と反対の面と隣接する側面の任意の一面に渡って形成する。 次に、 光— 電子変換部 2 1 4, 電子—光変換部 2 1 5, キヤリャ輸送部 2 1 6 を順 次積層する。 その後、 光の出口を除いて絶縁層 2 1 4 を形成する。 最後 に、 光の出口から絶縁層を跨いでシンチレータの側面の内、 はじめの電 極を形成した面以外から任意の面に渡って電極 2 1 3 を形成する。 光増 幅部へのバイアスの印加は、 シンチレ一タの側面の電極を利用して行う。 第 6図は、 本発明の一実施例のアレイ用検出素子への給電方法を示す 構成図である。 絶縁基板 2 1 9の両面に給電用のリ一ド 2 1 8 を取り付 け、 アレイ用検出素子 2 1の位置に対応した挿入口を設ける。 前述の如 く、 シンチレータの側面に電極を形成すれば、 リード 2 1 8 を介して光 増幅部への給電が可能になる。 リー ドは、 シンチレ一タの側面の電極に 所要の圧力で接触し、 電気的に接続するためであり、 特に図示した形状 に限るものでない。 第 7図は、 本発明の一実施例の二次元アレイ検出器を構成するアレイ 用検出素子を示す構成図である。 第 5図の如く有機多層膜により光増幅 部を実現する以外に、 ハイブリツ ドにより複数の機能素子を組み合わせ ることによつても同様の機能が達成できる。 たとえば、 フレキシブル基 板の片側に受光素子 2 5 3 を取り付け裏側を利用して増幅素子 2 5 4 と 発光素子 2 5 5 を取り付ける。 受光素子 2 5 3からの信号はフレキシブ ル基板 2 5 1 のスルーホールバタ一ンを使って反対側の増幅素子 2 5 4 に接続することができる。 増幅素子 2 5 4 と発光素子 2 5 5 との接続も 同様である。 受光素子 2 5 3は、 光学用接着剤 2 5 2によってシンチレ ータ 2 1 1 に取り付ける。 フレキシブル基板に形成した給電線のパター ンをシンチレ一タの側面まで延長することにより、 例えば、 前述の第 6 図の手法により各素子へ給電することができる。 FIG. 5 is a configuration diagram showing a detection element for an array constituting a two-dimensional array detector according to one embodiment of the present invention. The structure is the same as described in FIG. Here, a method for extending the electrode 2 13 to the side surface of the scintillator 2 11 will be described. For example, the electrode 2 13 on the scintillator side is formed over any one of the side surfaces adjacent to the surface opposite to the radiation incident surface. Next, the photo-to-electron converter 2 14, the electron-to-optical converter 2 15, and the carrier transporter 2 16 are sequentially stacked. After that, an insulating layer 214 is formed except for a light exit. Lastly, the electrodes 2 13 are formed over the insulating layer from the light exit to any surface from the side of the scintillator other than the first electrode. The bias is applied to the optical amplifier using the electrode on the side surface of the scintillator. FIG. 6 is a configuration diagram showing a method of supplying power to the array detection element according to one embodiment of the present invention. Power supply leads 218 are attached to both sides of the insulating substrate 219, and insertion holes corresponding to the positions of the array detection elements 21 are provided. As described above, if electrodes are formed on the side surfaces of the scintillator, power can be supplied to the optical amplifier via the leads 218. The lead contacts the electrode on the side surface of the scintillator with a required pressure and is electrically connected, and is not particularly limited to the illustrated shape. FIG. 7 is a configuration diagram showing a detection element for an array constituting a two-dimensional array detector according to one embodiment of the present invention. The same function can be achieved by combining a plurality of functional elements by hybrid, in addition to realizing the optical amplifier section by the organic multilayer film as shown in FIG. For example, the light-receiving element 253 is mounted on one side of the flexible substrate, and the amplifying element 254 and the light-emitting element 255 are mounted using the back side. The signal from the light receiving element 25 3 can be connected to the amplifying element 2 54 on the opposite side by using the through hole pattern of the flexible board 25 1. The same applies to the connection between the amplifying element 255 and the light emitting element 255. The light receiving element 25 3 is attached to the scintillator 2 11 with an optical adhesive 2 52. By extending the pattern of the power supply line formed on the flexible substrate to the side surface of the scintillator, power can be supplied to each element by, for example, the method shown in FIG.
第 8図は、 本発明の一実施例の線源側コリメータを示す斜視図である。 放射線発生装置 1 2 と放射線検出装置 2 6の相互の位置がずれていると、 透過画像において欠けが発生したり、 ぼけるなど分解能が低下する。 し たがって、 撮影の前にァライメン 卜が必要である。 ァライメント作業で は、 例えば、 中心に一個ピンホールの開いた調整用コリメ一タ 1 3 1 を 設置する。 この状態で測定を実施するとピンホールから出たパターン、 つまり、 1点にのみ出力が現れ、 その場所を特定することにより、 容易 に相互の位置関係を決定することができる。 これに基づいて、 放射線発 生装置 1 2 と放射線検出装置 2 6の位置合わせを行う。 調整用コリメ一 タは、 特異的なパターンを備えていることが必要で、 前述の如く、 中心 に一個のピンホール以外に、 複数のピンホールあるいは一個あるいは複 数のスリツ 卜を備えたものでも良い。 FIG. 8 is a perspective view showing a source-side collimator according to one embodiment of the present invention. If the positions of the radiation generating device 12 and the radiation detecting device 26 are shifted from each other, the resolution decreases, such as chipping or blurring in the transmitted image. Therefore, an alignment is required before shooting. In the alignment work, for example, an adjustment collimator 13 1 with one pinhole is installed at the center. When measurement is performed in this state, a pattern that comes out of the pinhole, that is, an output appears only at one point, and by specifying the location, the mutual positional relationship can be easily determined. Based on this, the radiation generator 12 and the radiation detector 26 are aligned. The adjustment collimator must have a specific pattern, as described above, even if it has multiple pinholes or one or more slits in addition to one pinhole at the center. good.
ァライメント作業が終了すると、 撮影用コリメータ 1 3 2に切り替え て撮影を行う。 切替機構は図示しないが、 スライ ド式, 回転式などが考 えられる。 When the alignment work is completed, switch to the collimator for shooting 1 3 2 To shoot. Although the switching mechanism is not shown, a sliding type or rotary type may be considered.
第 9図は、 本発明の一実施例の二次元の検出器出力を示す等高線グラ フである。 前述のピンホールコリメータの場合の二次元検出器からの出 力イメージである。 この結果からァライメン 卜の位置補正量、 例えば、 △ Xと Δ Υを決定し。 図示しないが、 放射線発生装置または放射線検出 装置の何れかまたは両方の姿勢制御手段によって位置補正する。 補正後、 再度測定し、 位置補正が正常に行われていることを確認しても良い。 第 1 0図は、 本発明の一実施例の二次元の検出器出力において検査体 の影響を補正する方法を示す説明図である。 一般的に、 ピンホールコリ メータの検出器出力において被検体の内部の影響により理想的なパター ンが得られるとは限らない、 例えば、 ほぼピンホールの中心に当たると ころに鉄骨などの内部構造物が入っていると、 理想的には、 同心円状の 等高線パターンが得られるところで、 片側半分が歪んだパターンになる。 これは、 歪んだ側が、 内部の鉄骨により放射線の強度が低下して起こる ものであり、 内部形状を正確に把握しない限りあらかじめ予測すること が不可能である。 しかしながら、 例えば、 線源強度を既知の異なる強度 にして測定するなどして、 二個以上の検出器出力のパターンを取得し、 例えば、 両者の対数の差を表示することにより検査体の内部構造の検査 結果への影響を補正することができる。 FIG. 9 is a contour graph showing a two-dimensional detector output of one embodiment of the present invention. It is an output image from a two-dimensional detector in the case of the pinhole collimator described above. From this result, the position correction amount of the alignment, for example, ΔX and ΔΥ are determined. Although not shown, the position is corrected by the attitude control means of one or both of the radiation generator and the radiation detector. After the correction, the measurement may be performed again to confirm that the position correction is performed normally. FIG. 10 is an explanatory diagram showing a method for correcting the influence of a test object on a two-dimensional detector output according to one embodiment of the present invention. In general, an ideal pattern is not always obtained due to the influence of the inside of the subject on the detector output of the pinhole collimator.For example, an internal structure such as a steel frame is almost at the center of the pinhole. When the pattern is included, ideally, a concentric contour pattern is obtained, and one half of the pattern becomes distorted. This is due to the fact that the distorted side causes the radiation intensity to decrease due to the internal steel frame, and it is impossible to predict in advance unless the internal shape is accurately grasped. However, for example, by measuring the source intensity at a known different intensity, two or more detector output patterns are acquired, and, for example, by displaying the logarithmic difference between the two, the internal structure of the test object is displayed. The effect on the test results can be corrected.
第 1 1 図は、 本発明の一実施例の一次元検出器型検査装置の線源側コ リメータおよび周辺を含む一次元検出器を示す構成図である。 駆動装置 2 8により回転可能な一次元のアレイ検出器 2 7の並進移動可能な有感 部の形状に対応させて線源 1 2側のコリメータ 1 4 1 のスリツ 卜の形状 を求める。 前記有感部はアレイ検出器 2 7の内部で並進移動可能な構造 になっている (第 1 2図, 第 1 3図, 第 1 4図でも同様である。 ) この とき、 放射線発生装置と放射線検査装置の相互の距離がスリッ 卜の寸法 に影響するので、 適切に選ぶ必要がある。 あるいは、 図示しないが、 ス リッ ト形状を可変にし、 撮影現場での条件に応じて最適に調整する。 検査体の形状と周辺の状況から必ずしも検出器の操作方向を同じにと ることができないことがある。 また、 検査体の内部形状によっては、 最 適な走査方向がある。 撮影時に、 走査方向を任意に取るためには、 線源 1 2側と検出器 2 7側の両方を同じく回転させる。 FIG. 11 is a configuration diagram showing a one-dimensional detector including a source-side collimator and its periphery of a one-dimensional detector type inspection apparatus according to one embodiment of the present invention. The shape of the slit of the collimator 144 on the side of the radiation source 12 is determined in accordance with the shape of the translatable sensitive part of the one-dimensional array detector 27 rotatable by the driving device 28. The sensitive part has a structure capable of translating within the array detector 27 (The same applies to Fig. 12, Fig. 13, and Fig. 14.) At this time, the mutual distance between the radiation generator and the radiation inspection device affects the dimensions of the slit. You need to choose. Alternatively, although not shown, the slit shape is made variable and adjusted optimally according to the conditions at the shooting site. The operating direction of the detector may not always be the same due to the shape of the test object and surrounding conditions. Also, there is an optimal scanning direction depending on the internal shape of the inspection object. In order to arbitrarily set the scanning direction during imaging, both the source 12 and the detector 27 are rotated in the same manner.
この装置でのァライメン 卜の手順は、 後述する (第 1 4図) 。 The procedure of alignment with this device will be described later (Fig. 14).
第 1 2図は、 本発明の一実施例の一次元検出器型検査装置の走査機構 および回転機構を示すための構成図である。 放射線発生部 1 1 では、 タ ーゲッ 卜から発生する放射線の中心軸とファンビ一ムコリメ一タ 1 4 2 の中心軸を概ね一致させ、 一次元アレイ検出器 2 7の走査に同期してフ アンビームコリメータの照射野を線源側の駆動装置 1 4によって移動す る。 ターゲッ 卜から発生する放射線は中心軸ほど強度が強く周辺になる ほど強度が弱くなる性質がある。 したがって、 ファンビームコリメータ 1 2のみを操作する場合は、 中心軸から離れた方向にファンビームコ リメ一タ 1 4 2が向いていると放射線の弱い部分を利用していることに なり、 撮影結果において周辺部の解像度を僅かに低下させる。 したがつ て、 ターゲッ 卜から発生する放射線の中心軸とファンビ一ムコリメータ の中心軸を概ね一致させて一次元アレイ検出器の走査に同期してファン ビームコリメータの照射野を移動することによリ、 周辺部での解像度の 低下を防止する。 線源側の駆動装置 1 4は、 ファンビ一ムコリメータ 1 2の照射野を一次元アレイ検出器 2 7の移動可能な有感部に概ね一 致させれば良いので、 放射線発生装置全体を一次元アレイ検出器に同期 して平行移動することによつても達成できる。 駆動装置 1 4により、 フ アンビームコリメ一タ 1 4 2 と駆動装置 2 8によリー次元アレイ検出器 2 7は、 独立にファンビームの中心に対して 9 0 ° 以上回転可能に構成 してある。 FIG. 12 is a configuration diagram showing a scanning mechanism and a rotation mechanism of the one-dimensional detector type inspection apparatus according to one embodiment of the present invention. In the radiation generator 11, the central axis of the radiation generated from the target and the central axis of the fan beam collimator 142 are substantially coincident with each other, and the fan beam is synchronized with the one-dimensional array detector 27 scanning. The irradiation field of the collimator is moved by the driving device 14 on the source side. The radiation generated from the target has the property that the intensity increases toward the center axis and decreases toward the periphery. Therefore, when operating only the fan beam collimator 1 2, if the fan beam collimator 1 4 2 is directed away from the central axis, the radiation weak part is used, and the imaging result , The resolution of the peripheral portion is slightly reduced. Therefore, the center axis of the radiation generated from the target and the center axis of the fan beam collimator are almost aligned, and the irradiation field of the fan beam collimator is moved in synchronization with the scanning of the one-dimensional array detector. To prevent the resolution from deteriorating at the periphery. Since the drive device 14 on the source side should make the irradiation field of the fan beam collimator 12 almost coincide with the movable sensitive part of the one-dimensional array detector 27, the entire radiation generator is primary. Synchronizes with the original array detector It can also be achieved by performing parallel movement. The drive device 14 allows the fan beam collimator 14 2 and the drive device 28 to independently rotate the three-dimensional array detector 27 by 90 ° or more with respect to the center of the fan beam. is there.
第 1 3図は、 本発明の一実施例の一次元検出器型検査装置の走査機構 を示すための構成図。 第 1 2図の方法に加えて、 ターゲッ トとファンビ —ムコリメータ 1 4 2 を同じく操作することでも実現できる。 ただし、 この場合には、 加速器の電子線の進行方向をタ一ゲッ 卜の手前で曲げる 等により電子線がターゲッ 卜の概ね同じ場所に概ね同じ角度で衝突する ようにしなければならない。 つま り、 例えば、 ターゲッ トの手前に電子 線を曲げる磁場発生装置 1 6 1 と自在継ぎ手 1 6 2 を取り付けることに よって実現できる。 FIG. 13 is a configuration diagram showing a scanning mechanism of the one-dimensional detector type inspection apparatus according to one embodiment of the present invention. In addition to the method shown in Fig. 12, this can also be achieved by operating the target and fan beam collimator 142 in the same way. However, in this case, the electron beam must be made to collide with the target at substantially the same angle at approximately the same angle by bending the traveling direction of the electron beam of the accelerator before the target. In other words, for example, it can be realized by attaching a magnetic field generator 161 that bends an electron beam and a universal joint 162 before the target.
第 1 4図は、 本発明の一実施例の一次元検出器型検査装置におけるァ ライメン 卜方法を示す説明図である。 FIG. 14 is an explanatory view showing an alignment method in the one-dimensional detector type inspection apparatus according to one embodiment of the present invention.
この装置での、 ァライメントの手順を示す。 例えばはじめに、 ファン 方向を図示しないコリメータ 1 4 1側の回転機構によって垂直に設定す るとともに、 一次元アレイ検出器のアレイ方向を検出器側回転機構 2 8 によって水平に設定して放射線を照射する。 これにより、 1 回目の一次 元アレイ検出器からの検出パターンを得る。 この検出パターンから水平 方向の位置補正量を得る。 次に、 ファン方向を水平, 一次元アレイ検出 器のアレイ方向を垂直に設定して放射線を照射して、 2回目の一次元ァ レイ検出器からの検出パターンを得る。 この検出パターンから水平方向 の位置補正量を得る。 以上、 2回の照射によりァライメン卜に必要な補 正量を決定する。 This section describes the alignment procedure for this device. For example, at first, the direction of the fan is set vertically by the rotating mechanism on the side of the collimator 14 (not shown), and the array direction of the one-dimensional array detector is set horizontally by the rotating mechanism 28 on the detector to irradiate radiation. . As a result, the first detection pattern from the one-dimensional array detector is obtained. The position correction amount in the horizontal direction is obtained from this detection pattern. Next, the fan direction is set to be horizontal, and the array direction of the one-dimensional array detector is set to be vertical, and radiation is applied to obtain a detection pattern from the second one-dimensional array detector. The position correction amount in the horizontal direction is obtained from this detection pattern. As described above, the correction amount necessary for the alignment is determined by the two irradiations.
第 1 5図は、 本発明の一実施例の一次元の検出器出力を示すグラフで ある。 ファンビ一ムコリメータの場合の一次元検出器からの出力ィメ一 ジである。 三つの山は、 ファンビームの照射方向を中心と両側 2ケ所の 3方向について測定したことに対応する。 この結果からァライメン 卜の 位置補正量、 例えば、 Δ Χと Δ Υを決定し。 図示しないが、 放射線発生 装置または放射線検出装置の何れかまたは両方の姿勢制御手段によって 位置補正する。 補正後、 再度測定し、 位置補正が正常に行われているこ とを確認しても良い。 FIG. 15 is a graph showing a one-dimensional detector output of one embodiment of the present invention. is there. This is an output image from a one-dimensional detector in the case of a fan beam collimator. The three peaks correspond to the measurement of the irradiation direction of the fan beam in the three directions of the center and two places on both sides. From this result, the position correction amount of the alignment, for example, ΔΧ and ΔΥ are determined. Although not shown, the position is corrected by the attitude control means of one or both of the radiation generator and the radiation detector. After correction, measurement may be performed again to confirm that the position correction has been performed normally.
第 1 6図は、 本発明の一実施例の二次元の検出器出力において検査体 の影響を補正する方法を示す説明図である。 第 1 5図と同様に三つの山 は中心と両側 2ケ所の 3方向について測定したことに対応する。 二次元 アレイ検出器とピンホールコリメ一タを用いた場合と同様に、 一般的に, 検出器出力パターンにおいて被検体の内部の影響により理想的なバタ一 ンが得られるとは限らない。 例えば、 ほぼファンビームの中心に当たる ところに鉄骨などの内部構造物が入っていると、 理想的には、 左右対称 な山形パターンが得られるところで、 片側半分が歪んだパターンになる ; これは、 歪んだ側が、 内部の鉄骨により放射線の強度が低下して起こる ものであり、 内部形状を正確に把握しない限りあらかじめ予測すること が不可能である。 しかしながら、 例えば、 線源強度を既知の異なる強度 にして測定し、 二個以上の検出器出力のパターンを取得し、 例えば、 両 者の対数の差を表示することにより検査体の影響を補正することができ る。 FIG. 16 is an explanatory diagram showing a method for correcting the influence of a test object on a two-dimensional detector output according to one embodiment of the present invention. As in Fig. 15, the three peaks correspond to the measurements in three directions: the center and two places on both sides. As in the case of using a two-dimensional array detector and a pinhole collimator, in general, an ideal pattern cannot always be obtained due to the influence of the inside of the subject in the detector output pattern. For example, if there is an internal structure such as steel frame near the center of the fan beam, ideally a symmetrical chevron pattern will be obtained, and one side will be distorted ; On the other hand, the radiation intensity decreases due to the internal steel frame, and it is impossible to predict in advance unless the internal shape is accurately grasped. However, for example, by measuring the source intensity to a known different intensity, acquiring two or more detector output patterns, and compensating for the effect of the test object, for example, by displaying the logarithmic difference between the two. be able to.
なお、 光ファイバ一を、 二次元イメージの伝送手段として使用可能で ある。 多数のファイバ一を使用して、 光ファイバ一同士の相対的な位置 関係を保持することによリ入り口での発光パターンをそのまま出口まで 伝送することができる。 そこで、 面状シンチレータあるいは多数のシン チレータを二次元配列した放射線検出部の発光ィメ一ジを多数の光ファ ィバーによって、 二次元 C C Dカメラなどの撮像素子に接続できる。 産業上の利用可能性 It should be noted that the optical fiber can be used as a means for transmitting a two-dimensional image. By using a large number of fibers and maintaining the relative positional relationship between the optical fibers, the light emission pattern at the entrance can be directly transmitted to the exit. Therefore, a planar scintillator or many scintillators The light emission image of the radiation detecting unit in which the chillers are two-dimensionally arranged can be connected to an image sensor such as a two-dimensional CCD camera by using a large number of optical fibers. Industrial applicability
本発明の第 1 の特徴によれば、 放射線検出装置の軽量化に有効で、 放 射線検査装置の機動力を高めることができる。 さらに、 有機多層膜型の 光増幅素子を利用することによリ、 蒸着等の薄膜形成技術が使用でき、 多数のシンチレ一タを一度に処理することで、 コス 卜の削減ができる。 本発明の第 2の特徴によれば、 ピンホールコリメータなどの調整用コ リメ一タにより放射線発生装置と放射線検査装置が分離していても簡便 なァライメン 卜の手段を得る。 また、 調整用コリメータはピンホールあ るいはスリッ 卜とすることで不要な照射を防止できる。 ADVANTAGE OF THE INVENTION According to the 1st characteristic of this invention, it is effective in reducing the weight of a radiation detection apparatus, and can enhance the mobility of a radiation inspection apparatus. Furthermore, by using an organic multi-layer type optical amplifying element, a thin film forming technique such as evaporation can be used, and the cost can be reduced by processing a large number of scintillators at once. According to the second feature of the present invention, simple alignment means can be obtained even when the radiation generator and the radiation inspection apparatus are separated by an adjusting collimator such as a pinhole collimator. Unnecessary irradiation can be prevented by using a pinhole or a slit for the adjustment collimator.
本発明の第 3の特徴によれば、 前述の第 2の特徴の効果に加えて、 一 次元アレイ検出器を回転させた状態で撮影することにより検査体の形状 あるいは撮影場所の状況に応じた走査方向を選択することによリ、 最良 の透過像を得ることができる。 According to the third aspect of the present invention, in addition to the effect of the above-mentioned second aspect, by taking an image while rotating the one-dimensional array detector, it is possible to adapt to the shape of the inspection object or the situation of the imaging place By selecting the scanning direction, the best transmitted image can be obtained.
本発明の第 4の特徴によれば、 ファンビ一ムコリメータを回転させ一 次元アレイ検出器のアレイ方向と概ね直角に保ちデータを取得すること によリ放射線発生装置と放射線検査装置が分離していても簡便なァライ メン 卜の手段を得る。 また、 ファンビームコリメ一タは不要な照射を防 止できる。 さらに、 一次元アレイ検出器を回転させた状態で撮影するこ とによリ検査体の形状あるいは撮影場所の状況に応じた走査方向を選択 することにより、 高品質の透過像を得ることができる。 According to the fourth feature of the present invention, the radiation generator and the radiation inspection apparatus are separated by rotating the fan beam collimator and acquiring the data while keeping the angle substantially perpendicular to the array direction of the one-dimensional array detector. Even simpler means of alignment can be obtained. In addition, the fan beam collimator can prevent unnecessary irradiation. In addition, high quality transmission images can be obtained by selecting the scanning direction according to the shape of the inspection object or the situation of the imaging location by taking an image while rotating the one-dimensional array detector. .
本発明の第 5の特徴によれば、 前述の第 4の特徴の効果に加えて、 タ —ゲッ 卜から発生する放射線の中心軸とファンビームコリメータの中心 軸を概ね一致させて一次元アレイ検出器の走査に同期してファンビーム コリメ一タの照射野を移動することにより、 周辺部での放射線強度が弱 いことが原因とする解像度の低下を防止できる。 According to the fifth aspect of the present invention, in addition to the effect of the fourth aspect, the center axis of the radiation generated from the target and the center of the fan beam collimator are obtained. By moving the irradiation field of the fan beam collimator synchronously with the scanning of the one-dimensional array detector with the axes substantially aligned, resolution degradation due to weak radiation intensity at the periphery is prevented. it can.
以上のように、 放射線発生装置と、 検査体を挟んで対向する位置に配 置する放射線検出装置からなる放射線検査装置において、 放射線検出装 置を二次元アレイ検出器で構成する場合に、 アレイ検出器の放射線の入 射面と対向する面に光増幅素子を備える。 また、 コリメータをァライメ ン ト作業時と撮影時で切り替える。 放射線検出装置を一次元アレイ検出 器で構成する場合に、 コリメータおよび検出器を独立に回転可能とする。 二次元アレイ検出器型放射線検査装置において、 検査の効率が向上する。 また、 同じ装置で様々な寸法の構造物の検査ができる。 一次元アレイ検 出器型放射線検査装置において、 同じ装置で様々な寸法の構造物の検査 ができる。 また、 構造物に応じて走査方向を選べるので、 高品質の透過 像を得ることができる。 さらに、 不要な放射線の照射を低減する。 As described above, in a radiation inspection apparatus including a radiation generation apparatus and a radiation detection apparatus disposed at a position facing each other with an inspection object interposed therebetween, when the radiation detection apparatus is configured by a two-dimensional array detector, the array detection is performed. An optical amplification element is provided on the surface of the vessel facing the radiation incidence surface. The collimator is switched between alignment work and shooting. When the radiation detector is composed of a one-dimensional array detector, the collimator and the detector can be rotated independently. In a two-dimensional array detector type radiographic inspection system, inspection efficiency is improved. In addition, the same equipment can inspect structures of various dimensions. With a one-dimensional array detector-type radiation inspection system, structures of various dimensions can be inspected with the same device. In addition, since the scanning direction can be selected according to the structure, a high-quality transmission image can be obtained. In addition, reduce unnecessary radiation exposure.
Claims
Priority Applications (2)
| Application Number | Priority Date | Filing Date | Title |
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| JP2000515172A JP3918430B2 (en) | 1997-10-03 | 1997-10-03 | Radiation inspection equipment |
| PCT/JP1997/003547 WO1999018428A1 (en) | 1997-10-03 | 1997-10-03 | Radiographic inspection apparatus |
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| Application Number | Priority Date | Filing Date | Title |
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| PCT/JP1997/003547 WO1999018428A1 (en) | 1997-10-03 | 1997-10-03 | Radiographic inspection apparatus |
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| WO1999018428A1 true WO1999018428A1 (en) | 1999-04-15 |
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Cited By (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2010197179A (en) * | 2009-02-24 | 2010-09-09 | Central Res Inst Of Electric Power Ind | Radiation detection device, and nondestructive inspection device having the same |
| JP2010203808A (en) * | 2009-02-27 | 2010-09-16 | Central Res Inst Of Electric Power Ind | Non-destructive inspection method and non-destructive inspection system |
| JP2015225053A (en) * | 2014-05-30 | 2015-12-14 | 株式会社日立製作所 | X-ray imaging system and x-ray imaging method |
| JP2018200256A (en) * | 2017-05-29 | 2018-12-20 | 株式会社高速道路総合技術研究所 | Inspection method and performance determination method of laminated rubber support containing metal plug |
| CN115406916A (en) * | 2022-11-02 | 2022-11-29 | 北京紫方启研科技有限公司 | Split type X-ray detection system and method for realizing large-area detection |
Citations (8)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5372673A (en) * | 1976-12-10 | 1978-06-28 | Aloka Co Ltd | Radiation distribution detector using afterglow scintillator |
| JPS57179151U (en) * | 1981-05-09 | 1982-11-13 | ||
| JPS61172038A (en) * | 1985-01-28 | 1986-08-02 | Hitachi Ltd | Internal diagnostic device for objects |
| JPH05253309A (en) * | 1992-03-13 | 1993-10-05 | Mitsubishi Electric Corp | Radiation therapeutic apparatus |
| JPH0580906B2 (en) * | 1985-11-14 | 1993-11-10 | Pin Uan Shii | |
| JPH05302997A (en) * | 1992-04-27 | 1993-11-16 | Hitachi Ltd | Inspection method for radioactive waste solid and formation method for it |
| JPH05322802A (en) * | 1992-05-20 | 1993-12-07 | Nippon Steel Corp | X-ray CT system |
| JPH06233831A (en) * | 1993-02-10 | 1994-08-23 | Hitachi Medical Corp | Stereotaxic radiotherapeutic device |
-
1997
- 1997-10-03 WO PCT/JP1997/003547 patent/WO1999018428A1/en not_active Ceased
- 1997-10-03 JP JP2000515172A patent/JP3918430B2/en not_active Expired - Fee Related
Patent Citations (8)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5372673A (en) * | 1976-12-10 | 1978-06-28 | Aloka Co Ltd | Radiation distribution detector using afterglow scintillator |
| JPS57179151U (en) * | 1981-05-09 | 1982-11-13 | ||
| JPS61172038A (en) * | 1985-01-28 | 1986-08-02 | Hitachi Ltd | Internal diagnostic device for objects |
| JPH0580906B2 (en) * | 1985-11-14 | 1993-11-10 | Pin Uan Shii | |
| JPH05253309A (en) * | 1992-03-13 | 1993-10-05 | Mitsubishi Electric Corp | Radiation therapeutic apparatus |
| JPH05302997A (en) * | 1992-04-27 | 1993-11-16 | Hitachi Ltd | Inspection method for radioactive waste solid and formation method for it |
| JPH05322802A (en) * | 1992-05-20 | 1993-12-07 | Nippon Steel Corp | X-ray CT system |
| JPH06233831A (en) * | 1993-02-10 | 1994-08-23 | Hitachi Medical Corp | Stereotaxic radiotherapeutic device |
Non-Patent Citations (1)
| Title |
|---|
| APPLIED PHYSICS, Vol. 64, No. 10, (1995), MASAHIRO HIRAMOTO, TADASHI KATSUME & MASAAKI YOKOYAMA, "Optical Amplifier Having Organic Multilayer Thin-Firm Structure (in Japanese)", pages 1036-1039. * |
Cited By (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2010197179A (en) * | 2009-02-24 | 2010-09-09 | Central Res Inst Of Electric Power Ind | Radiation detection device, and nondestructive inspection device having the same |
| JP2010203808A (en) * | 2009-02-27 | 2010-09-16 | Central Res Inst Of Electric Power Ind | Non-destructive inspection method and non-destructive inspection system |
| JP2015225053A (en) * | 2014-05-30 | 2015-12-14 | 株式会社日立製作所 | X-ray imaging system and x-ray imaging method |
| JP2018200256A (en) * | 2017-05-29 | 2018-12-20 | 株式会社高速道路総合技術研究所 | Inspection method and performance determination method of laminated rubber support containing metal plug |
| CN115406916A (en) * | 2022-11-02 | 2022-11-29 | 北京紫方启研科技有限公司 | Split type X-ray detection system and method for realizing large-area detection |
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