Method for correcting the stacking phenomenon applied to X-ray spectrums acquired using a spectrometric sensor

US9689994B2 · US · B2

Patent metadata
FieldValue
Publication numberUS-9689994-B2
Application numberUS-201013512485-A
CountryUS
Kind codeB2
Filing dateNov 30, 2010
Priority dateNov 30, 2009
Publication dateJun 27, 2017
Grant dateJun 27, 2017

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Abstract

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A method correcting a measured spectrum of X radiation, according to a number of channels Nc, each channel i corresponding to an energy range between E i and Ei+ΔE i , including: determining function δt i,j (k) determining size of temporal deviation Δt interval separating two interactions with energy E i and E j , stacking of which leads to a detected energy value E k ; determining, from the function δt i,j (k), probability function P i,j (k) that an event counted in a channel k corresponds to a stack of two interactions, respectively of energies E i and E j ; determining, from the probability function P i,j (k), a stack spectrum as a part of the measured spectrum that corresponds only to the stacks alone; and calculating or estimating at least a first corrected spectrum, by the difference between the measured spectrum and the stack spectrum.

First claim

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The invention claimed is: 1. A method for correcting a measured spectrum of X radiation according to a number of channels Nc, each channel i corresponding to an energy range between E i and E i +ΔE i , comprising: determining, using processing circuitry, a function δt i,j (k), which defines a size of a temporal deviation Δt interval, such that two interactions with energy E i and E j temporally separated by Δt are stacked and considered to have a detected energy value E k ; determining, using the processing circuitry, from the function δt i,j (k), a probability function P i,j (k) that an event counted in a channel k corresponds to a stack of two interactions, respectively, of energies E i and E j ; calculating, using the processing circuitry, from the probability function P i,j (k), a stack spectrum, which is a part of the measured spectrum that corresponds only to the stack; and adjusting, using the processing circuitry, the measured spectrum based on a difference between the measured spectrum and the calculated stack spectrum thus forming at least a first corrected spectrum accounting for perturbations present in the measured spectrum due to a stacking phenomenon. 2. The method according to claim 1 , the stack spectrum being calculated from the measured spectrum, exposure time, dead time data, and a minimum duration, separating two photons, below which there is stacking of the two photons and only one of the two photons is detected. 3. The method according to claim 2 , the dead time being determined by simulation or experimentally. 4. The method according to claim 1 , further comprising iteratively calculating N it (N it ≧1) corrected spectrums, each iteration calculating a corrected spectrum of order (n) from a corrected spectrum of order (n−1) or from the measured spectrum if there is no preceding corrected spectrum of order (n−1), by calculating a difference between the corrected spectrum of order (n−1), or the measured spectrum, and the stack spectrum, wherein 1≦n≦N it , n is an integer, and N it corresponds to a number of iterations of said calculating. 5. The method according to claim 4 , further comprising, iterated N it times, with N it ≧1: calculating, using processing circuitry, a mean stacking probability, as a function of a preceding corrected spectrum Sp cor(n-1) , or of the measured spectrum if there is no preceding corrected spectrum, and exposure time and dead time data; estimating, using processing circuitry, the stack spectrum, as a function of the preceding corrected spectrum, or of the measured spectrum if there is no preceding corrected spectrum, and the exposure time; and calculating, using processing circuitry, the corrected spectrum, using the difference between a preceding corrected spectrum or the measured spectrum, and the estimated stack spectrum. 6. The method according to claim 5 , the mean stacking probability being calculated using formula: P mean = 1 - ( 1 - 2 × T dead T expo ) ∑ j = 1 N ⁢ ⁢ max ⁢ Sp cor ⁡ ( n - 1 ) ⁡ ( j ) where Sp cor(n-1) (j) is the value, for the channel j, of the preceding corrected spectrum SP cor(n-1) , or of the measured spectrum if there is no preceding corrected spectrum. 7. The method according to claim 1 , the stack spectrum being calculated using formula: Emp ⁢ ( k ) = ∑ i = 1 Nc ⁢ ∑ j = i Nc ⁢ P i , j ⁡ ( k ) . 8. The method according to claim 7 , wherein: P i , j ⁡ ( k ) = 1 - [ 1 - 2 × δ ⁢ ⁢ t i , j ⁡

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Classifications

  • G01T1/171Primary

    Compensation of dead-time counting losses · CPC title

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What does patent US9689994B2 cover?
A method correcting a measured spectrum of X radiation, according to a number of channels Nc, each channel i corresponding to an energy range between E i and Ei+ΔE i , including: determining function δt i,j (k) determining size of temporal deviation Δt interval separating two interactions with energy E i and E j , stacking of which leads to a detected energy value E k ; determining, from the …
Who is the assignee on this patent?
Rinkel Jean, Brambilla Andrea, Dinten Jean-Marc, and 2 more
What technology area does this patent fall under?
Primary CPC classification G01T1/171. Mapped technology areas include Physics.
When was this patent published?
Publication date Tue Jun 27 2017 00:00:00 GMT+0000 (Coordinated Universal Time) (B2). Legal status and post-grant events are not shown on this page.
What related patents are in patentsdb?
We list 8 related publications on this page (citations in our corpus or others sharing the same primary CPC).