Material identification using x-rays

• US 5,524,133 A
• Filed: 06/13/1994
• Issued: 06/04/1996
• Est. Priority Date: 01/15/1992
• Status: Expired due to Term

• Current Assignee: Smiths Heimann GmbH
• Original Assignee: Cambridge Imaging Limited
• Inventors: Ansorge, Richard E., Neale, William W., Rushbrooke, John G.
• Primary Examiner(s): WONG, DON KITSUN
• Application Number:
  US08/244,872
• Time in Patent Office: 722 Days
• Field of Search: 378/70, 378/71, 378/53, 378/83, 378/88, 378/90, 378/46, 378/51, 378/56, 378/44, 378/45, 378/46, 378/48, 378/5, 378/6, 378/7, 378/8, 378/57, 378/76, 250/393, 250/395
• US Class Current: 378/53
• CPC Class Codes: G01N 23/04 and forming images of the material
• CPC Class Codes: G01V 5/224 Multiple energy techniques using one type of radiation, e.g. X-rays of different energies

Abstract

A method and apparatus for detecting the mean atomic number of a mass of material, for example freight in a vehicle comprises: subjecting the mass to X-rays and determining the mean number N_A passing therethrough; subjecting the mass to higher energy X-rays and determining the new mean number N_B ; and determining the mean atomic number of the mass from look-up tables against the computed ratio N_A /N_B. The mass, such as a railway wagon, may be scanned by two linear accelerators arranged perpendicular to each other, detector arrays being disposed respectively opposite the accelerators, so that a three dimensional image can be built up of the mass.

Claims

1. A method of detecting the mean atomic number of a mass of material within a container comprising the steps of:

(a) subjecting the material to high energy X-rays and determining the mean number N_A of X-rays transmitted through a region thereof,

(b) separately and simultaneously subjecting the same region of the material to X-rays having a significantly higher energy than the first mentioned X-rays and determining the mean number N_B of the higher energy X-rays transmitted therethrough,

(c) computing the value of the ratio N_A to N_B, and

(d) determining from a look-up table and delivering as an output the average atomic number corresponding to the computed value of the N_A /N_B ratio.

2. A method according to claim 1 in which separate X-ray sources and X-ray detectors are employed, spaced apart so as to reduce cross-talk and interaction therebetween, and either one or both of the values of N_A (obtained from the source detector combination operating at the lower energy level) and N_B (obtained from the source detector combination operating at the higher energy level), is/are stored as appropriate to be available for the ratio computation step.

3. A method according to claim 1 in which a single broad energy band X-ray source is employed to project a range of high energy X-rays of 1 MeV and above towards the material (e.g. the container).

4. A method according to claim 3 in which a composite detector is placed beyond the material which, on bombardment by transmitted X-rays produces substantially simultaneously a first component predominantly attributable to the higher energy component of the incident X-rays, and a second component predominantly attributable to the lower energy component of the incident X-rays;

the energies carried by the said two components is determined;

numerical values relating thereto are generated;

a ratio is computed of one numerical value relative to the other; and

, using a look-up table as aforesaid, the mean atomic number for the material through which the X-rays have passed is derived therefrom, using the value of the said ratio.

5. A method according to claim 4 in which the products of Compton scattering in the target/convertor in the composite detector and electron-positron pair production are preferentially detected in separate crystals.

6. A method according to claim 4 in which photons attributable to higher energy X-rays transmitted through the material are preferentially detected by detecting rearwardly propagated annihilation photons attributable to electron-positron pair production in the target, typically at an angle of 135°

and greater.

7. A method according to claim 5 in which the preferential detection is enhanced by removing lower energy photons from the rearwardly propagating photons by filtering, as by using a sheet of lead or tungsten or like material, and forcing all the rearwardly propagating photons to pass therethrough, so that only the higher energy photons reach the second detector.

8. Apparatus for performing the method according to claim 5 comprising an x-ray source, a target/convertor, typically of tungsten, and two crystals located so as to separately receive forwardly propagating photons in the range 30°

to 60°

off the axis and to receive rearwardly propagating photons in the range 135°

to 180°

off the axis.

9. Apparatus for performing the method according to claim 1, comprising an x-ray source and a sandwich of absorbers and scintillators enabling an electromagnetic cascade to be sampled at depths from the end of the sandwich on which X-rays are incident.

10. Apparatus according to claim 9 in which the first element on which the X-ray beams impinges comprises a relatively thin crystal, so that the energy deposited is more or less independent of X-ray energy and the spectrum of sampled X-rays is therefore strongly peaked around 1 MeV, and the thin crystal is followed by a low-z beam hardener which preferentially removes lower energy X-rays from the beam, which is then transmitted to a series of high-z converters (which favour pair production) which alternate with and are thereby sandwiched by thin crystals which sample the electrons produced by collisions upstream of the crystals.

11. Apparatus according to claim 10 in which light from the crystals is conveyed to a photo-electric device using optical fibres.

12. Apparatus according to claim 10 in which the outputs from all the crystals are optically coupled to give a single optical output to the photo-electric device.

13. A freight checking facility incorporating at least one X-ray source/detector combination as claimed in claim 9, and means for computing the ratios of detector output signals from each detector and determining the mean atomic number of the material exposed to the X-rays, and further comprising:

(a) a housing or building surrounding the X-ray source(s) and X-ray detectors for absorbing any X-rays not absorbed by the material under test or by the detectors,

(b) entrance and exit doors;

(c) a path leading to the entrance, extending through the housing or building and leaving through the exit which in the housing or building extends between the source(s) and the detectors, to enable freight to move into, through and out of the housing or building;

(d) at least two paths beyond the exit with means for diverting freight which has been scanned onto one or the other of the two paths, the length of each of the two paths being such as to permit all of a group of linked items of freight to be contained wholly thereon;

(e) means by which freight from either of said two paths can be moved onto a single ongoing path beyond the section containing at least two paths; and

(f) means for preventing at least one item of freight from leaving the path onto which it has been conveyed if an alarm signal gathered in response to the earlier scanning of the freight on that path;

whereby an item of freight which has to be physically checked because of what has been seen during the scanning, need not impede the ongoing progress of other items of freight which do not cause alarm signals to be generated.

14. A facility according to claim 13 further comprising a linear accelerator operating at approximately 10 MeV together with various targets and beam hardeners is a collimator to define a fan beam of small width of the order of a few millimeters, and a path such as a railway track, roadway or conveyor extending perpendicular to the axis of the beam at a distance of typically 10 meters from the source target.

15. A facility according to claim 14 and further comprising another collimator located on the other side of the path to eliminate scattered X-rays which are not within the width of the fan, and an array of converters situated beyond the second collimator, crystals and absorbers being arranged in a manner so as to reduce cross-talk between one crystal and another to a level of approximately one part in one thousand, and optical fibre means (or electrical conductor means if the crystals generate electrical signals) leading to a device by which each crystal output can be scanned in turn and a value obtained therefrom corresponding to the X-ray photon population incident on the crystal concerned.

16. A facility according to claim 13 further comprising means programmed to generate an alarm signal in the event that certain ratio values are detected (for example corresponding to drugs, explosives and the like) or certain combinations of ratio values are detected within the same freight container.

17. An x-ray analysis device for determining the mean atomic number of an object by locating a broad band X-ray source on one side of a testing station and a detector on the other side, comprising:

a target having X-ray detectors positioned adjacent thereto, one of the detectors being positioned and adapted to receive X-rays scattered by the detector target in a generally rearward direction back towards the source and up to 45°

off the rearward axis and the other detector being positioned and adapted to detect forwardly propagating X-rays scattered off axis typically by more than 30° and

by less than 60°

thereto, due to so-called Compton scatter, each of the X-ray detectors providing signals proportional to the number of X-ray photons incident thereon;

means responsive to the two detector outputs forming a ratio of the number of photons detected by the two detectors and forming a numerical value thereof;

a look-up table containing information pertaining to given numerical ratios for different materials;

means for determining from the look-up table the information corresponding to the numerical ratio obtained from the outputs of the two detectors; and

means for delivering the said information as an output signal.

18. A device according to claim 17 in which the target is formed from tungsten, and the X-ray detectors are crystals of zinc tungstate or cadmium tungstate, the X-ray photons being converted by the crystals into electromagnetic radiation in the visible range, and the photons of visible light being detected and quantified using a photo-electric sensor adapted to generate from the light emitted from the crystal an electric current which can be measured to give a numerical value proportional to the X-ray photon population incident on the appropriate crystal.

19. A device according to claim 18 in which light emitting crystals are employed, light collection means being provided to gather light emitted by each crystal, and a light guide means such as optical glass or plastic fibres, for conveying the light to an intensified CCD camera or the like.

20. A device according to claim 19 in which an intensified CCD camera is employed where the light guide means from a large number of detectors in the array terminate at differently addressable points over the surface of the CCD camera, so that very low light levels and therefore X-ray emissions are detected using the light integrating properties of such a device.

21. A device according to claim 19 further comprising means for scanning after a suitable period of time has elapsed to permit integration of photons arriving thereon.

22. A device according to claim 17 in which the X-ray source is a conventional 10 MeV electron linear accelerator with targets and beam hardeners to determine the X-ray spectrum emanating therefrom.

23. A device according to claim 17 in which the X-rays from the source are collimated into a divergent but narrow beam which can be likened to a fan extending in a generally vertical plane from the point source, and a plurality of detectors are positioned in an array in the same vertical plane on the remote side of a testing station each pointing towards the source and preferably to the point from which the fan of X-rays emanates, and each distanced therefrom by approximately the same length, the two X-ray sensitive crystals associated with each detector being separately addressable to determine the photon population seen by them, for determining the ratio as aforesaid for each detector, means being provided for memorising the ratio obtained from each detector to enable a profile to be produced of all of the ratios seen by all of the detectors in the array.

24. A device according to claim 23 in which the detectors are arranged in two or more (typically four or five) different arcs also centred on the same point (e.g. the X-ray source) but having successively increased radii of curvature, and locating adjoining detectors on different ones of the arcs.

25. A device according to claim 17 further comprising means for introducing relative movement between the analysis device and the object, generally perpendicular to the plane of the X-ray beam, so that the object can effectively be scanned from one end to the other, and means for memorising the signals obtained during the lengthwise scanning, so that a two-dimensional profile can be obtained for the whole object as viewed by the detector.

26. A device according to claim 25 in which the object is mobile and the source and the detector array are aligned and fixed in position while the object is moved steadily therebetween, the source and detector array being located either on opposite sides of the object, or above and below the object.

27. A device according to claim 17 comprising a second source/detector combination located perpendicular to the first source/detector combination, so that the narrow beam of the second source propagates through the object in the same (or a parallel) plane as that occupied by the first beam but with the central axes of the two beams at right angles.

28. A device according to claim 27 in which the first source and detector array is located on opposite sides of the testing station, the second source is located above, and the second detector array below, the testing station, so that a composite profile of the object can be obtained for each of the inspected slices, across its width, as well as from top to bottom thereof.

29. A device according to claim 28 in which the object is rectilinear and the signals corresponding to the two profiles are stored, so that they can be employed to control a visual display to allow cross-sections of the object to be displayed showing material variation therein as viewed from side to side, from top to bottom, and from end to end.

30. A device according to claim 28 in which the signals are combined to permit a series of three-dimensional isometric views of the object to be displayed, with the nearside end face in each object corresponding to the cross-section that would be seen if the object were to be cut in two in a vertical plane and the nearer portion of the container removed, thereby leaving a cut face of the object exposed.

31. A device according to claim 28 further comprising means for comparing the image data in each slice with the next slice to determine any image content which is constant and appears in the same position in each slice, and enhancing the data relating thereto in the final image, or rendering the date invisible.

32. A method of detecting the mean atomic number of a mass of material within a container comprising the steps of:

(a) subjecting the material to high energy X-rays on the order of 1 MeV and determining the mean number N_A of X-rays transmitted through a region thereof,

(b) subjecting the same region of the material to X-rays having a significantly higher energy than the first mentioned X-rays, said higher energy being at least about 5 MeV, and determining the mean number N_B of the higher energy X-rays transmitted therethrough,

(c) computing the value of the ratio N_A to N_B, and

(d) determining from a look-up table and delivering as an output the average atomic number corresponding to the computed value of the N_A /N_B ratio.