JP5060410B2 - Radiation detector - Google Patents

Description

  The present invention relates to a radiation detection apparatus for measuring a one-dimensional or two-dimensional radiation intensity distribution used in a radiation handling facility such as a nuclear power plant.

  FIG. 23 is a diagram illustrating a basic configuration of an X-ray imaging apparatus disclosed in Patent Document 1. Hereinafter, a technique for measuring a two-dimensional distribution of radiation intensity based on FIG. 23 will be described. First, a large number of fluorescent fibers 17 (wavelength shift fibers) are arranged so as to be orthogonal to the back side of the X-ray incident surface of the plate-like scintillator 1 that generates light due to the incidence of radiation, and an XY two-dimensional matrix. Enable to output information. The fluorescent fiber 17 absorbs scintillation light, emits longer wavelength fluorescent light, and can transmit it.

When scintillation light is generated at the radiation incident position, a part of the scintillation light is absorbed by the intersecting fluorescent fibers 17 and converted into fluorescence. The fluorescence propagates through the fluorescent fiber 17 and is detected by a photodetector attached to the end face of the fluorescent fiber 17. Then, the intersection of the light-detected fluorescent fibers 17 in the X and Y directions is identified as the radiation incident position.
JP 7-72565 A

  In the example described above, a high positional resolution substantially equal to the diameter of the fluorescent fiber 17 can be obtained by arranging the fluorescent fibers 17 in a “dense” manner, but conversely, the number of the fluorescent fibers 17 is reduced so as to be spaced apart from each other. When arranged “sparse”, the encounter probability of scintillation light to the fluorescent fiber 17 is lowered, and as a result, the signal detection probability is remarkably lowered.

  In the case of X-ray imaging, since a relatively high resolution is required, there is no problem. However, in the case of measuring the distribution of radioactive materials and radiation intensity in a general nuclear power plant, the case of X-ray imaging It is often preferable to be able to measure a larger area with a coarser resolution than

  For example, assuming the collective distribution measurement of an area of several tens of centimeters with a minimum division area of about 10 cm square, and applying the method of Japanese Patent Laid-Open No. 7-72565, the number of fluorescent fibers 17 is reduced and “sparse” In the case of the arrangement, effective detection sensitivity cannot be achieved, and in the case of arrangement in a dense manner, a large number of photodetectors and signal processing circuits are required, which is not practical.

  In addition, for detectors used in nuclear facilities and the like, radiation components are always present in the background other than the measurement target, so it is important to be able to compensate for these, and it is important to measure large areas and against background radiation. It is essential to achieve both correction and compensation.

  An object of the present invention is to provide a radiation detection apparatus that can cope with a position identification type measurement of a large area and can perform background compensation.

  In order to solve the above problems and achieve the object, the radiation detection apparatus of the present invention is configured as follows.

The radiation detection apparatus of the present invention includes a plate-like scintillator that generates light due to incidence of radiation, a plurality of first light guides that are disposed on a side surface of the scintillator and include a phosphor therein, and the first internal are arranged parallel to the plane of the plate-shaped scintillator opposite the light detecting means, with respect to the plane radiation incident on the plate-shaped scintillator for detecting the light guide is disposed on the end face fluorescence converted light And a plurality of second light guides including a phosphor, and a light detection means for detecting the fluorescence-converted light that is disposed in each of the plurality of second light guides , and is disposed in the first light guide. Further, it is characterized in that the simultaneity of the signals of the light detecting means and the light detecting means arranged in the second light guide is inspected.

  According to the radiation detection apparatus of the present invention, position identification type measurement in a large area is possible, and correction and compensation under various background conditions can be performed with a minimum apparatus configuration.

  Hereinafter, embodiments of the present invention will be described with reference to the drawings. In each embodiment, the same elements are denoted by the same reference numerals, and redundant description is omitted.

(First embodiment)
FIG. 1 is a perspective view showing the configuration of the position identification type radiation detection apparatus according to the first embodiment of the present invention. 1 includes a plate-like scintillator 1 that generates light due to incidence of radiation, a first light guide 2 that includes a phosphor inside, a second light guide 3 that includes a phosphor inside, And the photodetector 4.

  A first light guide 2 is connected to each of the two side surfaces of one scintillator 1, and the scintillator 1 is disposed on the opposite side (below the scintillator 1 in the figure) to the surface on which the radiation enters the scintillator 1. Three second light guides 3 are arranged in parallel so as to be parallel to the surface. The photodetectors 4 are connected to the end faces of the first light guide 2 and the second light guide 3, respectively.

  Hereinafter, the operation principle of the radiation detection apparatus will be described. When radiation enters the scintillator 1, scintillation light is generated in the scintillator 1. The scintillation light is divided into internal propagation light that propagates inside the scintillator 1 and is absorbed by the first light guide 2, and a component that radiates to the outside simultaneously with light emission.

  The light that has reached the first light guide 2 and has undergone fluorescence conversion is captured and transmitted inside the first light guide 2 and is incident on the photodetector 4 mounted on the end face. On the other hand, the scintillation light emitted into the air without being captured by the scintillator 1 hits the second light guide 3 arranged immediately below, and is converted into fluorescence here. The fluorescence generated in the second light guide 3 is captured and diffused in the second light guide 3 and detected by the photodetector 4 mounted on the end face.

  Wherever scintillation light is generated in the scintillator 1, signal detection is performed via the first light guide 2 disposed on the side surface. However, light emitted into the air is emitted from the light emitting point, and One of the two light guides 3 will be encountered. Therefore, one-dimensional (three-region) position information can be obtained by examining the simultaneity of the signals of the scintillator 1 and the three second light guides 3.

  The scintillator 1 is a flat plate. As the 1st light guide 2 and the 2nd light guide 3, what processed the resin containing the fluorescent material called a wavelength shifter, or an optical fiber etc. can be used.

  The first light guide 2 shown in FIG. 1 is obtained by polishing a resin containing a wavelength shifter into a prismatic shape and is not flexible compared to an optical fiber, but is processed into an arbitrary thickness. Is possible. In addition, since the first light guide 2 is surrounded by an air layer having a large refractive index difference from the resin, the internal light capture / transmission efficiency is high, and the first light guide 2 can be thickened to increase the fluorescence conversion probability of scintillation. When there are restrictions on the shape of the scintillator 1 or the connection position of the photodetector 4, it is preferable to use an optical fiber for the first light guide 2.

  As for the type of the wavelength shifter, it is necessary to select one that overlaps the emission wavelength band of the scintillator 1 and the absorption wavelength band of the wavelength shifter. A part of the fluorescence generated in the first light guide 2 and the second light guide 3 due to the fluorescence conversion action is captured inside and transmitted to the end face, so that the fluorescence is detected by arranging the photodetector 4 there. can do.

  For general plastic scintillators that emit light in the 400 nm band, a wavelength shifter and several types of optical fibers including the same are commercially available, including BC-482A manufactured by Bikeron and Y-7 manufactured by Kuraray.

  In order to closely bond the first light guide 2 or the second light guide 3 and the photodetector 4, an optical binder is generally used. This optical binder reduces reflection loss by preventing the air layer from intervening. Although not specifically shown, a reflective material is applied to or attached to the open side surfaces of the scintillator 1 and the second light guide 3. This is a general measure useful for securing the amount of light collection.

  2 to 8 are diagrams showing examples of the arrangement of the photodetectors. 2 to 6 are plan views, and FIGS. 7 and 8 are front views. As an arrangement method of the photodetector 4 connected to the first light guide 2, there is a method of connecting to all end faces of all the first light guides 2 as shown in FIG. This method is most advantageous from the viewpoint of detection efficiency although the number of detection units 4 is large.

  Further, as shown in FIGS. 3 and 4, it is possible to arrange the photodetector 4 only on one end surface with respect to one first light guide 2. In this case, as shown in FIG. 5, attaching a reflector 5 that reflects fluorescence to an open end where the photodetector 4 is not disposed is an effective means for securing a light collection amount. As the reflector 5, either a specular reflector or an irregular reflector can be applied.

As shown in FIG. 4, it is also possible to arrange the photodetector 4 after making the length of the first light guide 2 shorter than the length of the side surface of the scintillator 1. It may be necessary to take such measures from the viewpoint of mounting space. In this case, the reduction rate f of the condensed light amount is
f = 1− (the length of contact between the first light guide 2 and the side surface of the scintillator 1)
/ (Side length of scintillator 1)
You can predict that. Also in this case, the system shown in FIG. 6 to which the reflector 5 described above is added is practical.

  Furthermore, some specific examples of the connection between the scintillator 1 and the first light guide 2 can be considered. When the first light guide 2 utilizing the difference in refractive index with air as shown in FIG. 1 is used, as shown in FIG. 7A, the scintillator 1 and the first light guide are simply used. As shown in FIG. 7B, a method is considered in which a groove is formed in the first light guide 2 and the scintillator 1 is fitted therein. The method of using the groove has an advantage that it is easy to fix when mounting is considered.

  In addition, as described above, the first light guide 2 can be used other than the prisms surrounded by the air layer in some cases, and as shown in FIGS. 8A and 8B, the first light guide 2 is cylindrical. May be good. 8A shows a case where the scintillator 1 and the first light guide 2 are simply put together, and FIG. 8B shows a case where a groove is formed in the first light guide 2, The case where the scintillator 1 is fitted is shown. Further, as shown in FIG. 8C, a fiber-shaped one with a clad on the first light guide 2 may be used.

(Second Embodiment)
FIG. 9 is a perspective view showing a configuration of a position identification type radiation detection apparatus according to the second exemplary embodiment of the present invention. 9 includes a plate-like scintillator 1 that generates light due to incidence of radiation, a first light guide 2 that includes a phosphor inside, a second light guide 3 that includes a phosphor inside, And the photodetector 4.

  A first light guide 2 is connected to each of two sides of the three scintillators 1 arranged in the same plane, and is opposite to a surface on which radiation is incident on the three scintillators 1 (in the figure, the scintillator 1), the three second light guides 3 are juxtaposed in the same plane so that the surfaces of the scintillators 1 are parallel to each other and the longitudinal direction thereof is orthogonal to the longitudinal direction of the scintillators 1. Yes. Further, a photodetector 4 is connected to each first light guide 2 and each second light guide 3.

  That is, the scintillator 1 and the second light guide 3 constitute a 3 × 3 matrix. Then, by checking the coincidence of the signal detection information at the end of the first light guide 2 connected to each scintillator 1 by the light detector 4 and the signal detection information at the second light guide 3, nine sections (3 X3) position identification capability can be provided.

  10 and 11 are front views showing examples of arrangement of the first light guide 2 and the scintillator 1. When arranging a plurality of scintillators 1 side by side, there is a method of providing the first light guides 2 on both sides of each scintillator 1 as shown in FIG.

  However, as shown in FIG. 11, a method of condensing two scintillators 1 by using one first light guide 2 is also conceivable. In consideration of the balance between the cross-sectional area of the first light guide 2 and the size of the light-sensitive surface of the photodetector 4 to be used, the method of FIG. Light can be received and the number of photodetectors 4 can also be suppressed.

(Third embodiment)
FIG. 12 is a perspective view showing a configuration of a position identification type radiation detection apparatus according to the third embodiment of the present invention. The radiation detection apparatus shown in FIG. 12 is formed into a two-layered structure in which the light that is captured and diffused inside the scintillator 1 is collected by the first light guide 2 disposed on the side surface of the scintillator 1 in parallel in the same direction. It is structured.

  According to the third embodiment, different line types can be recognized in the first layer and the second layer, and one-dimensional position identification can be performed.

(Fourth embodiment)
FIG. 13 is a perspective view showing a configuration of a position identification type radiation detection apparatus according to the fourth exemplary embodiment of the present invention. In the radiation detection apparatus of FIG. 13, the structure shown in FIG. 12 in the third embodiment is further opposite to the first layer (upper layer) with respect to the second layer (lower layer) (three layers of the second layer). Below the scintillator 1, the three second light guides 3 are parallel to each scintillator 1 and the longitudinal direction thereof is orthogonal to the longitudinal direction of each scintillator 1 (that is, each first light They are arranged side by side (perpendicular to the guide 2). Further, a photodetector 4 is connected to each second light guide 3.

  According to the fourth embodiment, as in the case shown in FIG. 9, one layer of the scintillator 1 and one layer of the second light guide 3 form a pair and operate as a two-dimensional detector. However, the second light guide 3 can provide one-dimensional information for position detection to the two scintillator 1 layers in common without doubling the apparatus of FIG.

  Conventionally, when a two-dimensional detector is formed in two layers for background correction and compensation, it has been essential to have a double device configuration. However, according to this configuration, the second light guide 3 is shared. Therefore, it is possible to realize a two-dimensional background correction / compensation function while performing a two-dimensional measurement with a simple structure.

(Fifth embodiment)
FIG. 14 is a perspective view showing a configuration of a position identification type radiation detection apparatus according to the fifth exemplary embodiment of the present invention. In the radiation detection apparatus of FIG. 14, with respect to the structure shown in FIG. 9 in the second embodiment, a flat plate is formed on the surface of each second light guide 3 facing the scintillator 1 side of the first layer. A scintillator (plastic scintillator) 1 is disposed in close contact.

  Since the scintillator 1 is attached to the second light guide 3, the scintillator 1 located at the upper part in FIG. 14 receives light emitted into the air to emit fluorescence, and radiation is applied to the attached scintillator 1 itself. Fluorescence is also generated when incident.

  Since the scintillator 1 uses two layers as described above, it is possible to perform one-dimensional background correction and compensation using a difference in line type, energy, and the like, and the second light guide 3 has different generation factors. Are detected by the common photodetector 4, the number of components can be reduced, and the entire apparatus can be simplified.

  That is, according to the fifth embodiment, a one-dimensional background correction / compensation function can be realized while performing two-dimensional measurement with a simpler structure.

(Sixth embodiment)
FIG. 15 is a perspective view showing a configuration of a position identification type radiation detection apparatus according to the sixth exemplary embodiment of the present invention. In the radiation detection apparatus of FIG. 15, as in the structure shown in FIG. 14 in the fifth embodiment, a flat scintillator (plastic scintillator) 1 is adhered and adhered to the surface of each second light guide 3. However, the position of the surface to be bonded is opposite to that in the case of FIG. 14 and is the opposite side to the surface facing the scintillator 1 side of the first layer, that is, the back surface. In this case, since the second light guide 3 is interposed between the two scintillator 1 layers, the degree of radiation transmission differs.

  As an example, a mixed field of γ rays and β rays is assumed. In the case of FIG. 14, there may be a case where a part of the energy is lost in the first layer scintillator 1 that passes first and the remaining energy is lost in the second layer scintillator 1. When β rays having energy that can be transmitted through the first scintillator 1 are incident, there is a probability of coincidence of the first scintillator 1 and the second scintillator 1, but during this time as shown in FIG. When the second light guide 3 is interposed, energy loss without light emission occurs in the second light guide 3. For this reason, when the thickness of the second light guide 3 is adjusted so that all of the remaining energy minus the energy loss in the first layer is lost in the second light guide 3, the scintillator 1 of the second layer is adjusted. Then, β rays are shielded. Using these effects, the systems shown in FIGS. 14 and 15 can be selected for the purpose of background correction and compensation according to the measurement target.

(Seventh embodiment)
16 to 18 are front views showing examples of arrangement of the first light guide 2 and the scintillator 1 according to the seventh embodiment of the present invention. In the layout method of the first light guide 2 described above, when one light guide 2 is common to two scintillators 1 as shown in FIG. 16, the two scintillators 1 are not optically separated from each other.

  For this reason, for example, the light of the left scintillator 1 in FIG. 16 is transmitted without being absorbed by the first light guide 2 located in the center in FIG. 16 and propagates to the right scintillator 1. However, there is a small probability. In this case, in the rightmost first light guide 2 in FIG. 16, there is a possibility that the signal from the left scintillator 1 is erroneously detected as the signal from the adjacent right scintillator 1.

  Therefore, in the seventh embodiment, when one light guide 2 is common to two scintillators 1 as shown in FIG. 17, the light guide 2 shields light transmission between the light guides 2. By inserting a reflector 5 that prevents propagation and reflects light, the two scintillators 1 can be optically separated. As the reflector constituting the reflector 5, an aluminum vapor-deposited sheet or a material coated with irregular reflectors such as titanium oxide or magnesium oxide can also be used.

  However, it is difficult to include such a reflector 5 in the light guide 2 from the viewpoint of processing. Therefore, as shown in FIG. 18, two light guides 21 and 21 having a half thickness of the first light guide 2 arranged at both ends in the figure are used to sandwich the reflector 5 between these gaps. The method is a realistic policy.

  According to the seventh embodiment, it is possible to reduce the event of erroneously detecting the light emission of the adjacent scintillator 1.

(Eighth embodiment)
FIG. 19 is a block diagram showing a configuration of a position identification type radiation detection apparatus according to the eighth exemplary embodiment of the present invention. In the following description including the eighth embodiment, the names of the AND processing unit and the OR processing unit are used, but the AND processing takes the logical product of the input signals and simultaneously detects and outputs the signal. Only “true” is output, and the OR processing unit takes a logical sum of the input signals, and “true” is output when any signal is detected and output. The inversion processing unit inverts the logic of the signal and has a function of outputting “false” when the input signal is detected / outputted and outputting “true” when the input signal is not detected.

  In FIG. 19, as shown in FIG. 5 or FIG. 6, one light beam is applied to each first light guide 2 mounted on the side surface of the first layer scintillator 1 arranged on the radiation incident surface side. It is assumed that the detector 4 is connected. The outputs of these two photodetectors 4 are input to the first AND processing unit 6.

  Each of the first light guides 2 mounted on the side surface of the second layer scintillator 1 is also connected to the photodetector 4 one by one, and the output thereof is sent to the second AND processing unit 7. Have been entered.

  The output of the first AND processing unit 6 is a signal indicating the radiation incidence / detection timing in the first layer scintillator 1, and the output of the second AND processing unit 7 is the radiation in the second layer scintillator 1. It is a signal which shows incident / detection timing. By using the first AND processing unit 6 or the second AND processing unit 7 according to the arrangement of the photodetectors 4, the signal from the scintillator 1 sandwiched between the two first light guides 2 is used. Can be obtained.

  In FIG. 19, two photodetectors 4 are connected to the second light guide 3. The detector outputs from the two photodetectors 4 are input to the first OR processing unit 8 as signals corresponding to the detection of the fluorescence generated when the light from the scintillator 1 is incident on the second light guide 3. ing. Information indicating that fluorescence is generated in the second light guide 3 is obtained from the output from the first OR processing unit 8. Since the first scintillator 1 shares the first light guide 2 with other scintillators, AND processing is necessary, but the second light guide 3 is optically independent of each other. Therefore, OR processing is possible.

  The first-layer scintillator 1 and the second-layer scintillator 1 are arranged in the same direction, but the second light guide 3 is arranged orthogonal to these scintillators 1 so as to correspond to rows and columns. Has been. Therefore, as a whole, the number of position identifications corresponding to (number of scintillators 1 per layer) × (number of second light guides 3) is realized.

  For this reason, by inputting the output of the first AND processing unit 6 and the output of the first OR processing unit 8 to the third AND processing unit 9, the first layer is output as the output of the third AND processing unit 9. It is possible to detect the light emission of the first scintillator 1, that is, the incidence of radiation, in the region where the scintillator 1 and the corresponding second light guide 3 intersect. Similarly, addition of position information related to the second scintillator 1 from the output of the fourth AND processing unit 10 that receives the output of the second AND processing unit 7 and the output of the first OR processing unit 8 as inputs. The obtained radiation detection information is obtained.

(Ninth embodiment)
FIG. 20 is a block diagram showing a configuration of a position identification type radiation detection apparatus according to the ninth exemplary embodiment of the present invention. In FIG. 20, one photodetector 4 is connected to each first light guide 2 mounted on the side surface of the scintillator 1 disposed on the radiation incident surface side, as shown in FIG. 5 or FIG. It is assumed that

  Outputs from these two photodetectors 4 are input to the first AND processing unit 6. The output of the first AND processing unit 6 is a signal indicating the radiation incidence / detection timing in the first scintillator 1. With the arrangement of the photodetectors 4, information indicating that the signal is from the scintillator 1 sandwiched between the two first light guides 2 can be obtained by using the first AND processing unit 6.

  In FIG. 20, two photodetectors 4 are connected to the second light guide 3. The detector outputs from the two photodetectors 4 are input to the first OR processing unit 8 as signals corresponding to the detection of the fluorescence generated when the light from the scintillator 1 is incident on the second light guide 3. ing. Information indicating that fluorescence is generated in the second light guide 3 is obtained from the output from the first OR processing unit 8.

  The second light guide 3 is arranged so as to correspond to rows and columns orthogonal to the scintillator 1 installed on the radiation incident side. Therefore, as a whole, the number of position identifications corresponding to (the number of scintillators 1 per layer) × (the number of second light guides) is realized.

  Therefore, by inputting the output of the first AND processing unit 6 and the output of the first OR processing unit 8 to the third AND processing unit 9, the output of the third AND processing unit 9 can be used as the output of the scintillator 1. It is possible to detect light emission of the scintillator 1, that is, incidence of radiation in a region where the corresponding second light guide 3 intersects.

(Tenth embodiment)
21 and 22 are block diagrams showing the configuration of the position identification type radiation detection apparatus according to the tenth embodiment of the present invention. In the eighth and ninth embodiments, in order to explain the position identification method, the output of the first AND processing unit 6 is all treated as effective as the first layer detection signal.

  Hereinafter, embodiments for background correction and compensation will be described. First, it is assumed that the surface contamination of devices, articles, bodies, etc. by β nuclides is measured. In this case, first, surrounding background γ-ray components are to be corrected and compensated. The way of thinking at this time will be described.

If the detection layer on the radiation incident surface side is the first layer and the next detection layer is the second layer, both β rays and γ rays are mainly detected in the first layer, and mainly γ is detected in the second layer. A line is measured. Measure for a certain time, and let the count rate detected in the first layer be (β + γ) and the count rate detected in the second layer be γ ′,
β = (β + γ) −c1 · γ ′ (c1 = calibration coefficient)
As a result, a β-ray count rate obtained by correcting the γ-ray component is obtained.

  In either case of FIG. 21 or FIG. 22, the outputs of the first AND processing unit 6 and the second AND processing unit 7 are respectively counted for a certain time and divided by the measurement time, so that (β + γ) and γ ′ are obtained. can get. This processing method can be applied as the simplest method.

  In general, it is practical to use a plastic scintillator for the scintillator 1, but the energy absorption (giving rate) of β rays is about 2 MeV per 1 cm of the scintillator. That is, if the thin scintillator 1 is used for the purpose of suppressing the γ-ray sensitivity, it can be easily predicted that the energy will be lost depending on the β-ray energy.

  Now, when the scintillator 1 is composed of a plastic scintillator having a thickness of about 1 mm to 2 mm, the energy absorption of β rays is 200 keV to 400 keV. In the case of Co-60 β-rays, the maximum energy is around 300 keV, so most of the energy is lost by the scintillator 1.

  However, when a β-ray component having higher energy is present in the background, the signal other than the signal to be counted from the output signals of the first AND processing unit 6 and the second AND processing unit 7 as described above. It is also necessary to exclude.

  For example, assume that the surface contamination of a wall or floor is measured. Common floor and wall materials contain K-40, which is a natural radioactive material, so that 1.3 MeV β-rays with relatively high energy are emitted. On the other hand, the β ray of Co-60, which can be a contamination source in nuclear facilities, is as low as 300 keV. All nuclides emit gamma rays. Therefore, it is considered to eliminate as much as possible the K-40 β-ray component having higher energy from the β-ray signal while correcting the γ-ray as in the previous example.

  Now, the β ray component of Co-60 is β1, and the β ray component of K-40 is β2. The γ-ray components are collectively expressed as γ. In this case, (β1 + β2 + γ) is included in the first detection signal, and (β2 + γ) is included in the second detection signal.

  However, with respect to β2, the probability that the first layer and the second layer are detected simultaneously is extremely high. On the other hand, since γ-rays react with plastics (interaction) only with a certain probability, and the reaction cross-section of a thin scintillator is small, the probability that γ-rays are detected simultaneously in the first and second layers. Is practically negligible.

  Taking advantage of this phenomenon, it is effective to remove in advance the detection signal for the first layer, assuming that the component counted simultaneously with the second layer is the β2 component. In FIG. 21 and FIG. 22, the fifth AND output is output from the first AND processing unit 6 as one input, and the output from the second AND processing unit 7 is input through the second inversion processing unit 13. By using the output of the AND processing unit 12 as the input of the third AND processing unit 9, the high energy β-ray component (β2) that clearly generated the signal in the second layer is excluded from the first layer output signal. can do. Thereby, by checking the count rate of the output of the third AND processing unit 9, the mixing ratio of β2 is reduced, and a measurement result closer to the true β1 component can be obtained.

  Further, as described above, it is necessary to consider the β2 component to be mixed into the detection component in the second layer. In order to obtain the β2 component, the output of the first AND processing unit 6 and the output of the second AND processing unit 7 which are the first and second layer signal outputs are input to the seventh AND processing unit 15. Are simultaneously detected by logical product, and the output and the output of the first OR processing unit 8 for adding position information are input to the eighth AND processing unit 16, and the β2 component is output as the output. Can be obtained.

  By using the output of the eighth AND processing unit 16, the β2 component is measured in the absence of the β1 component in advance, the mixing ratio of the β2 component to the first layer is checked, and correction is performed at the time of measurement. Techniques can also be applied.

  In order to perform measurement while excluding the β2 component, an output obtained by passing the output of the first AND processing unit 6 through the first inversion processing unit 11 and the output of the second AND processing unit 7 are used as a sixth AND. The input to the processing unit 14, the output thereof, and the output of the first OR processing unit 8 for adding position information are input to the fourth AND processing unit 10. Can get the dominant output.

  In this way, the third AND processing unit 9 reduces the influence of β2 and outputs the signal of the β1 line component to which the position information is added, and the fourth AND processing unit 10 reduces the influence of β2 and positions. The signal output of the γ-ray component to which the information is added, the eighth AND processing unit 16 is a signal output mainly composed of the β2 component and to which the position information is added.

  Therefore, when these output signals are counted and the count rate is obtained as a measurement result, the following processing is possible. If the measurement result of the third AND processing unit 9 is A (β1), the measurement result of the fourth AND processing unit 10 is A (γ), and the measurement result of the eighth AND processing unit 16 is A (β2), It is obvious that the more accurate value β (1) of β1 can be obtained by the following calculation.

A (β) = A (β1) −c1 · A (γ) −c2 · A (β2)
Here, c1 and c2 are calibration constants, c1 is the ratio of the first and second layers of γ-ray detection efficiency, and c2 is the detection efficiency ratio of the first and second layers to β2.

  The signal processing forms shown in FIGS. 21 and 22 can be applied to both cases, including cases where the measurement object is α rays and neutron rays under a γ background.

  Of course, the terminals connected from the first inversion processing unit 11 or the second inversion processing unit 13 are opened for the input terminals of the fifth AND processing unit 12 and the sixth AND processing unit 14 as necessary. It is also possible that a treatment that is always “true” is used by applying either or both of the fifth AND processing unit 12 and the sixth AND processing unit 14 at the same time. Further, the eighth AND processing unit 16 and the seventh AND processing unit 15 may not be used at all. These can be used in any combination depending on the measurement object and background conditions.

  In addition, this invention is not limited only to each said embodiment, In the range which does not change a summary, it can deform | transform suitably and can be implemented.

The perspective view which shows the structure of the position identification type | mold radiation detection apparatus which concerns on the 1st Embodiment of this invention. The figure which shows the example of arrangement | positioning of the photodetector which concerns on the 1st Embodiment of this invention. The figure which shows the example of arrangement | positioning of the photodetector which concerns on the 1st Embodiment of this invention. The figure which shows the example of arrangement | positioning of the photodetector which concerns on the 1st Embodiment of this invention. The figure which shows the example of arrangement | positioning of the photodetector which concerns on the 1st Embodiment of this invention. The figure which shows the example of arrangement | positioning of the photodetector which concerns on the 1st Embodiment of this invention. The figure which shows the example of arrangement | positioning of the photodetector which concerns on the 1st Embodiment of this invention. The figure which shows the example of arrangement | positioning of the photodetector which concerns on the 1st Embodiment of this invention. The perspective view which shows the structure of the position identification type | mold radiation detection apparatus which concerns on the 2nd Embodiment of this invention. The front view which shows the example of arrangement | positioning of the 1st light guide and scintillator which concern on the 2nd Embodiment of this invention. The front view which shows the example of arrangement | positioning of the 1st light guide and scintillator which concern on the 2nd Embodiment of this invention. The perspective view which shows the structure of the position identification type | mold radiation detection apparatus which concerns on the 3rd Embodiment of this invention. The perspective view which shows the structure of the position identification type | mold radiation detection apparatus which concerns on the 4th Embodiment of this invention. The perspective view which shows the structure of the position identification type | mold radiation detection apparatus which concerns on the 5th Embodiment of this invention. The perspective view which shows the structure of the position identification type | mold radiation detection apparatus which concerns on the 6th Embodiment of this invention. The front view which shows the example of arrangement | positioning of the 1st light guide and scintillator which concern on the 7th Embodiment of this invention. The front view which shows the example of arrangement | positioning of the 1st light guide and scintillator which concern on the 7th Embodiment of this invention. The front view which shows the example of arrangement | positioning of the 1st light guide and scintillator which concern on the 7th Embodiment of this invention. The block diagram which shows the structure of the position identification type | mold radiation detection apparatus which concerns on the 8th Embodiment of this invention. The block diagram which shows the structure of the position identification type | mold radiation detection apparatus which concerns on the 9th Embodiment of this invention. The block diagram which shows the structure of the position identification type | mold radiation detection apparatus which concerns on the 10th Embodiment of this invention. The block diagram which shows the structure of the position identification type | mold radiation detection apparatus which concerns on the 10th Embodiment of this invention. The figure which shows the basic composition of the X-ray imaging device which concerns on a prior art example.

Explanation of symbols

  DESCRIPTION OF SYMBOLS 1 ... Scintillator, 2 ... 1st light guide, 3 ... 2nd light guide, 4 ... Photodetector, 5 ... Reflector, 6 ... 1st AND processing part, 7 ... 2nd AND processing part, 8 ... 1st OR processing part, 9 ... 3rd AND processing part, 10 ... 4th AND processing part, 11 ... 1st inversion processing part, 12 ... 5th AND processing part, 13 ... 2nd inversion Processing part, 14 ... 6th AND processing part, 15 ... 7th AND processing part, 16 ... 8th AND processing part, 17 ... Fluorescent fiber, 21 ... Light guide.

Claims (1)

A plate-like scintillator that produces light due to the incidence of radiation;
A plurality of first light guides arranged on a side surface of the scintillator and including a phosphor inside;
A light detection means for detecting the fluorescence-converted light disposed on the end face of the first light guide;
A plurality of second light guides arranged in parallel to the surface of the plate-like scintillator on the opposite side to the surface on which radiation enters the plate-like scintillator and containing a phosphor inside;
A light detection means for detecting the fluorescence-converted light that is arranged in each of the plurality of second light guides,
A radiation detection apparatus for examining the simultaneity of signals of light detection means arranged in the first light guide and light detection means arranged in the second light guide.

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