Method and device for recognition of a material making use of its transmission function

Patent metadata

Field	Value
Publication number	US-9885674-B2
Application number	US-201013514802-A
Country	US
Kind code	B2
Filing date	Nov 2, 2010
Priority date	Dec 9, 2009
Publication date	Feb 6, 2018
Grant date	Feb 6, 2018

Abstract

A method for characterizing nature of a material, including: providing at least one sample of the material between an X-ray source and a detector; using the X-ray source to make N X-radiation spectra transmitted through the material, each for a time; calculating transmission function of the material as a function of energy or the detection channel; and in each of at least two energy zones, calculating the integral of the transmission function, thus forming at least a first transmission coefficient and a second transmission coefficient.

First claim

The invention claimed is:

1. A method for providing an improved characterization of a nature of a material and/or of a thickness of the material, comprising:
providing at least one object comprising the material between an X-ray source and a single detector;
using the X-ray source, obtaining at least one X-radiation spectrum of radiation transmitted through the object and impinging on the single detector for a time between about 1 ms and about 10 seconds and for a minimum fluence rate of incident photon radiation that is about 10 6 mm −2 s −1 to about 10 7 mm −2 s −1 , the at least one X-radiation spectrum of radiation representing an amplitude distribution of radiation pulses measured by the detector;
calculating, from the obtained at least one X-radiation spectrum, a transmission function of the material as a function of energy or of energy channel, from a ratio of an intensity of the radiation transmitted through the object to an intensity of radiation that is incident on the object;
selecting N different energy bands from the obtained at least one X-radiation spectrum for the calculated transmission function, N being greater than or equal to 2;
calculating, via at least one circuit or processor, a transmission coefficient corresponding to each of the selected N different energy bands by applying a statistical magnitude of the calculated transmission function in each of the selected N different energy bands,
said statistical magnitude being obtained by calculating an integral or an average of the calculated transmission function in a given energy band of said selected N different energy bands, and
said calculated transmission coefficient comprising a first transmission coefficient α1 corresponding to a first energy band of the selected N different energy bands and a second transmission coefficient α2 corresponding to a second energy band of the selected N different energy bands, said first and second transmission coefficients comprising coordinates (α1, α2) in an (α1, α2) plane; and

providing the improved characterization of the nature of the material and/or the thickness of the material, via the at least one circuit or processor, by comparing values of the coordinates (α1, α2) in the (α1, α2) plane with values of known coordinates of standard transmission coefficients (α standardmaterial1 , α standardmaterial2 ) in the (α1, α2) plane.

2. The method according to claim 1 , wherein the intensity of the radiation that is incident on the object is determined either in an absence of the object, or by calculation based on known emission parameters of the source.

3. The method according to claim 1 , wherein N is equal to 2, the method further comprising:
selecting a first energy zone as a low energy zone corresponding to the first energy band, and a second energy zone as a high energy zone corresponding to the second energy band,
wherein the calculating the integral or the average of the calculated transmission function is with respect to energy in order to obtain said statistical magnitude.

4. The method according to claim 3 , wherein the first energy zone is between 15 keV and 50 keV, and the second energy zone is between 50 keV and 120 keV.

5. The method according to claim 1 , wherein the minimum fluence rate of incident photon radiation is greater than 10 7 mm −2 s −1 .

6. The method according to claim 1 , wherein a number of the at least one radiation spectrum obtained is between 1 and 100.

7. The method according to claim 1 , wherein the providing the improved characterization of the nature and/or of the thickness of the material comprises using the calculated transmission coefficients corresponding to said each of the selected N different energy bands by positioning the calculated coefficients in a plane comprising known material coefficients as a function of their thickness.

8. The method according to claim 1 , wherein the comparison between the values of the coordinates (α1, α2) in the (α1, α2) plane with values of known coordinates of standard transmission coefficients (α standardmaterial1 , α standardmaterial2 ) in the (α1, α2) plane comprises a measurement of distance between a set of N transmission coefficients and each standard set of N transmission coefficients of each standard material, the nature of the material and/or the thickness of the material corresponding to a nature and/or a thickness of the standard material represented by the standard set of N transmission coefficients having closest coordinates.

9. The method according to claim 1 , further comprising a prior step of measuring an energy spectrum of radiation from the X-ray source when there is no material inserted between the source and the single detector.

10. The method according to claim 1 , further comprising a spectrum correction for disturbances resulting from stacking phenomena.

11. The method according to claim 1 , wherein the detector comprises a detector made of a CdTe or CdZnTe or CdMnTe, or HgI2, or AsGa, or Si, or TIBr semiconductor.

12. A device for the providing an improved characterization of a nature of a material and/or of a thickness of the material, comprising:
an X-ray source;
a single detector and an electronic circuit configured to obtain at least one X-radiation spectrum transmitted through an object comprising the object and impinging on the single detector for a time between about 1 ms and about 10 seconds and for a minimum fluence rate of incident photon radiation that is about 10 6 mm −2 s −1 to about 10 7 mm −2 s −1 , the at least one X-radiation spectrum of radiation representing an amplitude distribution of radiation pulses measured by the detector; and
at least one processing circuit configured to:
calculate, from the obtained at least one X-radiation spectrum, a transmission function of the material as a function of energy or of energy channel, from a ratio of an intensity of the radiation transmitted through the object to an intensity of radiation that is incident on the object,
calculate at least one transmission coefficient corresponding to each of N different selected energy bands from the obtained at least one X-radiation spectrum for the calculated transmission function, N being greater than or equal to 2, by applying a statistical magnitude of the calculated transmission function in each of the selected N different energy bands, said statistical magnitude being obtained by calculating an integral or an average of the calculated transmission function in a given energy band of said selected N different energy bands,
said calculated at least one transmission coefficient comprising at least a first transmission coefficient α1 corresponding to a first energy band of the selected N different energy bands and a second transmission coefficient α2 corresponding to a second energy band of the selected N different energy bands, said first and second transmission coefficients comprising coordinates (α1, α2) in an (α1, α2) plane, and
provide the improved characterization of the nature of the material and/or the thickness of the material by comparing values of the coordinates (α1, α2) in the (α1, α2) plane with values of known coordinates of standard transmission coefficients (α standardmaterial1 , α standardmaterial2 ) in the (α1, α2) plane.

13. The device according to claim 12 , wherein the intensity of the radiation that is incident on the object is determined either in an absence of the object, or by calculation based on known emission parameters of the source.

14. The device according to claim 12 , wherein N is equal to 2, the at least one processing circuit being further configured to calculate the integral or the aver

Assignees

• Ouvrier Buffet Patrice
• Beldjoudi Guillaume
• Rebuffel Veronique
• Rinkel Jean
• Commissariat Energie Atomique

Inventors

• Ouvrier Buffet Patrice
• Beldjoudi Guillaume
• Rebuffel Veronique
• Rinkel Jean

Classifications

• G01N23/087 Primary

  using polyenergetic X-rays · CPC title

• G01T1/171

  Compensation of dead-time counting losses · CPC title