CN200947086Y - Detector array and equipment - Google Patents
Detector array and equipment Download PDFInfo
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- CN200947086Y CN200947086Y CN 200620022987 CN200620022987U CN200947086Y CN 200947086 Y CN200947086 Y CN 200947086Y CN 200620022987 CN200620022987 CN 200620022987 CN 200620022987 U CN200620022987 U CN 200620022987U CN 200947086 Y CN200947086 Y CN 200947086Y
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Abstract
The utility model discloses a detector array which comprises: the first linear array of the first ray and the second ray of first plurality parts that are used to penetrate and detect the tested objects with the first ray and the second ray sent alternatively and the second linear detector of the first ray and the second ray of the second plurality parts that are used to penetrate and detect the tested objects; wherein, the first plurality part and the second plurality part are the same. The utility model can improve the scan and inspect efficiency and the material distinguishing accurate rate of the alternative dual energy ray.
Description
Technical field
The utility model relates to the detector that is used for the object radiation perspective imaging, be particularly related to the equipment of a kind of detector array and this detector array of use, with the edge that occurs in the process that eliminate to utilize the tested object of radiological survey X that alternately produces wrong identification and the inaccurate problem of identification, and can double to improve scanography efficient to object materials.
Technical background
Along with improving constantly that customs and safety check system require, utilize the X ray of two kinds of different-energies that tested object is carried out nondestructive inspection (NDI), realize simultaneously the technology that the material of tested object is discerned has been begun extensively to be promoted, as U.S. Pat 5,044,002.Recently, in the Non-Destructive Testing of large object, (＞1MeV) dual intensity method realizes that the technology of material identification is also proposed again, sees U.S. Pat 5,524,133 at high-energy section.
The dual intensity method realizes that the physical principle of material identification is, the X ray and the same object interaction of two bundle different-energies, there is difference in interaction because photon energy is different with object, can think simply that this difference is that general performance is the difference of attenuation coefficient ratio.Therefore,, the multiple method that alternately produces two kinds of different-energy X ray has been proposed based on this principle, as U.S. Pat 6,069,936 and the single radiographic source that discloses of International Application No. WO 00/43760, the way by absorbed modulates the high energy power spectrum.In addition, International Application No. WO 2004/030162 A2 has disclosed the ray that is alternately produced two kinds of power spectrums of height by an accelerator.But during this alternately property generation high and low power X ray scanning object, has a major defect: the X ray of two kinds of different-energies is the generations of certain frequency interleaved, produces between the two beam lines to have certain time interval.When being used for the scanning of tested object (Ru Hangbao, container etc.), scanned object be certain speed in operation, in the time interval that high and low power X ray produces, tested object will move certain distance.Like this, the two beam lines of high low energy and the process of matter interaction are not identical.Therefore, this will influence the accuracy to material identification, and especially in the edge of tested object, the ray that has two kinds of energy is and the phenomenon of different object interactions, obtains wrong recognition result thus.Simultaneously, the error that causes because of the interaction of high low energy ray and non-same substance in order to reduce, traditional method be, makes the movement velocity of tested object slower, and this will seriously limit examination of cargo efficient.And, still can't solve for the wrong identification problem of object edge.
The utility model content
In view of the above problems, finished the utility model.The purpose of this utility model is the system for discriminating materials that proposes a kind of detector array and use this detector array, utilizes the object edge wrong identification defective that causes in the checking process of ray to tested object that alternately produces to eliminate.
In first aspect of the present utility model, a kind of detector array has been proposed, comprise first ray of surveying more than first parts penetrating tested object and first linear array detector of second ray; And be arrangeding, survey first ray of more than second parts that penetrate described tested object and second linear array detector of second ray in parallel with described first linear array detector, wherein said more than first parts are identical with described more than second part part.
According to embodiment of the present utility model, described first linear array detector and described second linear array detector are closely arranged.
According to embodiment of the present utility model, the distance between described first linear array detector and described second linear array detector is adjustable.
According to embodiment of the present utility model, described distance depend on the movement velocity of tested object and alternately produce first ray and second ray between interval time.
According to embodiment of the present utility model, each of described first linear array detector and described second linear array detector comprises scintillation crystal or gas detector.
According to embodiment of the present utility model, described first linear array detector is connected with same treating apparatus with described second linear array detector.
According to embodiment of the present utility model, described first linear array detector and described second linear array detector are connected with separately treating apparatus respectively.
According to embodiment of the present utility model, described first ray and second ray are produced by same radiographic source.
According to embodiment of the present utility model, described scintillation crystal is cadmium tungstate or cesium iodide.
In addition, the utility model also provides a kind of equipment that comprises described detector array.
Detector array is surveyed hard radiation, and by the dislocation coupling, realizes interaction and accurate survey of high low energy beam to the object same position.Simultaneously, the distance that first linear array is surveyed between the device and second linear array detector was determined according to the time interval that the movement velocity and the radiographic source of tested object produces high low energy ray, thereby guarantee the ray behind high low energy ray and the same partial action of tested object is detected, improved the accuracy of dual intensity method, and eliminated the wrong identification of tested object edge material identification.Because the distance between first linear array detector and second linear array detector can be adjusted and make that the motion quick-action of tested object is variable, has reduced the requirement to the checking matter speed of moving body.In addition, because first linear array detector and second linear array detector while acquired signal be equivalent to increase detection area, and the small cross sections of single scintillator have guaranteed the detection accuracy to object, obtain meticulous detection image.
Description of drawings
Fig. 1 realizes the synoptic diagram of the system of material identification according to the detector array that utilizes of the utility model embodiment;
Fig. 2 is according to embodiment of the present utility model, when radiographic source alternately produces the ray of different energy, and the principle of work synoptic diagram of detector array;
Fig. 3 is the structural representation according to the detector array of the utility model embodiment.
Embodiment
The contrast accompanying drawing describes specific embodiment of the utility model in detail below.
Fig. 1 realizes the synoptic diagram of the system of material identification according to the biserial detector array that utilizes of the utility model embodiment.
As shown in Figure 1, comprise that by use the detector array of the first linear array detector 104a and the second linear array detector 104b realizes the dual intensity ray that radiographic source alternately produces is gathered.Radiographic source 100 can alternately produce the ray such as X ray.Synchro control part 105 provides synchronizing signal 110 to radiographic source 100 and the first linear array detector 104a and the second linear array detector 104b, makes the sequential of radiographic source 100 synchronizing signals 110 alternately produce high low energy ray.
The ray 102 that radiographic source 100 produces obtains fan-shaped planar radiation through after the collimating apparatus 101.Tested object 103 moves at the fixed-direction perpendicular to radiator plane with a fixing speed, as shown in Figure 1.Transmitted radiation after planar radiation and 103 effects of tested object is surveyed by the first linear array detector 104a and the second linear array detector 104b.Here, the first linear array detector 104a and the second linear array detector 104b are parallel to each other, and the synchronizing signal that provides according to synchro control part 105, and the parameter of adjusting Acquisition Circuit realizes synchronous acquisition, but this is not necessary.
Then, the processing module of biserial detector array is mated the signal of two rays of nearest collection, exports the probe value after high low energy ray and the 103 same position effects of tested object.This probe value is sent to Flame Image Process and material identification part 106 through network.Flame Image Process is passed through dual intensity algorithm and relevant image processing algorithm with material identification part 106, finally discerns the attribute of tested object materials, as inorganics, organism, heavy metal etc.
Fig. 2 is according to embodiment of the present utility model, when radiographic source 100 alternately produces the ray of different energy, and the principle of work synoptic diagram of detector array.
As shown in Figure 2, radiographic source 100 alternately produces the ray 102H and the 102L of high low energy according to sequential 203, and high low energy ray is with alternately emission of a fixed frequency, and launches two time interval t between the ray and equate.Object 103 moves to a direction with fixed speed V.Suppose random time, radiographic source 100 emission high-energy ray 102H, ray is through part 1 and part 2 effects of collimation back with tested object 103, ray after penetrating is gathered and buffer memory by the first linear array detector 104a and the second linear array detector 104b respectively, is expressed as 102H-1A and 102H-2B respectively.
Then, radiographic source 100 after the time, is then being launched low energy ray 102L through t.At this moment, tested object 103 travelled forward a pixel apart from V*t.After low energy ray 102L penetrates the part 2 and part 3 of tested object, gathered and buffer memory by the first linear array detector 104a and the second linear array detector 104b respectively, be expressed as 102L-2A and 102L-3B respectively.The processing module of detector array is matched the high-energy ray 102H and the probe value 102L-2A that gathers of the probe value 102H-2B that gathers of the part 2 effect back of tested object 103 and current low energy ray 102L and the part 2 effect backs of tested object 103 of buffer memory last time, exports to the Flame Image Process and the material identification part 106 of connection.
Next, radiographic source 100 produces high-energy ray 102H once more according to sequential 203, simultaneously tested object 103 moved once more a pixel apart from V*t, so the part 3 of high-energy ray 102H and tested object 103 and part 4 interactions.The first linear array detector 104a and the second linear array detector 104b gather the probe value after high- energy ray 102H and 103 interactions of tested object respectively, are expressed as 102H-3A and 102H4B.Then, the processing module of detector array is matched the low energy ray 102L and the part 3 of tested object 103 part 3 of probe value 102L-3B that the back gathers and current high-energy ray 102L and the tested object 103 probe value 102H-3A that the back gathers that interacts that interacts of buffer memory last time, exports to the Flame Image Process and the material identification part 106 of connection.Like this, along with the motion of tested object 103, realized the acquisition of signal after high low energy ray is to the same partial action of tested object 103.
Like this, owing to adopted two first and second parallel linear array detector 104a and 104b, first ray of the approximate narrow beam of a branch of high energy that radiographic source 100 produces earlier and the part 1 of tested object 103 and part 2 interact, and are gathered by the first and second linear array detector 104a and 104b then.First ray that penetrates the part 1 of tested object 103 is surveyed also first probe value of output 1 by the first linear array detector 104a, and first ray that penetrates the part 2 of tested object 103 is surveyed also first probe value of output 2 by the second linear array detector 104b.And then second ray of a branch of low energy of radiographic source 100 emission, this moment tested object 103 distance of a pixel that travelled forward, promptly this moment, second ray will be simultaneously interacts with the part 2 and 3 of tested object 103.The first linear array detector 104a and the second linear array detector 104b survey the signal of the second ray penetrating component 2 and 3 respectively, second probe value of output 2 and first probe value of part 3.At this moment, second probe value of first probe value of part 2 and part 2 just is respectively the output valve after first ray and second ray penetrate the part 2 of tested object 103.Therefore, just can determine the effective atomic number in the part 2 of tested object 103 according to its first probe value and second probe value, thus determine this part 2 material properties.
Here, two linear array detector 104a and 104b can be by adjacent two scintillators together, as cadmium tungstate (CdWO
4) or the cesium iodide formation, shown in Fig. 3 (A).Shown in Fig. 3 (A), the first and second linear array detector 104a and 104b can be combined into an integral body.Two scintillation crystals of every row are fixed, and connect processing module 305.Two crystal detect after the signal, while output signal 302A and 302B, these two signals are buffered and handle for 305 li in processing module, gathered the high low energy ray signal of twice adjacent pulse when detector after, processing module 305 is exported the high low energy probe value of tested object appropriate section to giving Flame Image Process and material identification part 106 after matching high low energy signal.But, also can allow the first linear array detector 104a and the second linear array detector 104b respectively independent output signal 301A and 301B to separately processing module (not shown).The ray that detector array whenever collects high energy or low energy penetrate tested object penetrate signal after just export to processing module 305, so that probe value is matched according to high low energy, thereby obtain the high low energy probe value of tested object 103 various pieces.Scheme as an alternative, each of two linear array detector 104a and 104b can be made of gas detector.
In addition, can regulate apart from d between the first linear array detector 104a and the second linear array detector 104b is shown in Fig. 3 (B).Here apart from the interval time t decision of d by the movement velocity V and the high low energy ray of radiographic source 100 generations of tested object 103, i.e. d=V*t.Just, the movement velocity that produces time interval between two rays of high low energy and tested object according to radiographic source is regulated the distance between this first linear array detector and second linear array detector, thereby satisfies the requirement that adjacent high low energy ray penetrates the same part of tested object.
The above; it only is the embodiment in the utility model; but protection domain of the present utility model is not limited thereto; anyly be familiar with the people of this technology in the disclosed technical scope of the utility model; the conversion that can expect easily or replacement all should be encompassed in of the present utility model comprising within the scope.Therefore, protection domain of the present utility model should be as the criterion with the protection domain of claims.
Claims (10)
1. a detector array is characterized in that, comprising:
Detection penetrates first ray of more than first parts of tested object and first linear array detector of second ray, and wherein second ray and first ray are alternately emissions; And
Be arranged, survey first ray of more than second parts that penetrate described tested object and second linear array detector of second ray in parallel with described first linear array detector, wherein said more than first parts are identical with more than second part part.
2. detector array as claimed in claim 1 is characterized in that, described first linear array detector and described second linear array detector are closely arranged.
3. detector array according to claim 1 is characterized in that, the distance between described first linear array detector and described second linear array detector is adjustable.
4. detector array according to claim 3 is characterized in that, described distance depend on the movement velocity of tested object and alternately produce first ray and second ray between interval time.
5. according to the described detector array of one of claim 2～3, it is characterized in that each of described first linear array detector and described second linear array detector comprises scintillation crystal or gas detector.
6. detector array according to claim 5 is characterized in that, described scintillation crystal is cadmium tungstate or cesium iodide.
7. detector array according to claim 5 is characterized in that, described first linear array detector is connected with same treating apparatus with described second linear array detector.
8. detector array according to claim 5 is characterized in that, described first linear array detector and described second linear array detector are connected with separately treating apparatus respectively.
9. detector array according to claim 5 is characterized in that, described first ray and second ray are produced by same radiographic source.
10. an equipment that comprises detector array is characterized in that, described detector array comprises:
Detection penetrates first ray of more than first parts of tested object and first linear array detector of second ray, and wherein second ray and first ray are alternately emissions; And
Be arranged, survey first ray of more than second parts that penetrate described tested object and second linear array detector of second ray in parallel with described first linear array detector, wherein said more than first parts are identical with more than second part part.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN 200620022987 CN200947086Y (en) | 2006-05-19 | 2006-05-19 | Detector array and equipment |
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| CN 200620022987 CN200947086Y (en) | 2006-05-19 | 2006-05-19 | Detector array and equipment |
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| CN200947086Y true CN200947086Y (en) | 2007-09-12 |
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Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| TWI400470B (en) * | 2009-10-30 | 2013-07-01 | Iner Aec Executive Yuan | Method for determining penetration effect and detecting efficiency and calibrating detecting efficiency of crystal |
| WO2020088198A1 (en) * | 2018-11-01 | 2020-05-07 | 同方威视技术股份有限公司 | Backscatter imaging system, scanning inspection system, and backscatter imaging method |
-
2006
- 2006-05-19 CN CN 200620022987 patent/CN200947086Y/en not_active Expired - Fee Related
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| TWI400470B (en) * | 2009-10-30 | 2013-07-01 | Iner Aec Executive Yuan | Method for determining penetration effect and detecting efficiency and calibrating detecting efficiency of crystal |
| WO2020088198A1 (en) * | 2018-11-01 | 2020-05-07 | 同方威视技术股份有限公司 | Backscatter imaging system, scanning inspection system, and backscatter imaging method |
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| Date | Code | Title | Description |
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| C14 | Grant of patent or utility model | ||
| GR01 | Patent grant | ||
| C56 | Change in the name or address of the patentee | ||
| CP03 | Change of name, title or address |
Address after: 100084 Tsinghua University, Beijing, Haidian District Co-patentee after: Nuctech Company Limited Patentee after: Tsinghua University Address before: 100084 Tsinghua University, Beijing, Haidian District Co-patentee before: Qinghua Tongfang Weishi Tech Co.,Ltd. Patentee before: Tsinghua University |
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| C17 | Cessation of patent right | ||
| CF01 | Termination of patent right due to non-payment of annual fee |
Granted publication date: 20070912 Termination date: 20130519 |