Method for detecting a moving radioactive source and associated device
US-2015346352-A1 · Dec 3, 2015 · US
US9739893B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-9739893-B2 |
| Application number | US-201414761466-A |
| Country | US |
| Kind code | B2 |
| Filing date | Jan 21, 2014 |
| Priority date | Jan 23, 2013 |
| Publication date | Aug 22, 2017 |
| Grant date | Aug 22, 2017 |
A practical reading order for non-experts. Skip the full description unless you need deep technical detail.
What the patent document calls the invention.
A short plain-language summary of the technical disclosure.
Who owns or filed the patent and who is credited as inventor.
Filing, priority, publication, and grant dates set the timeline.
The legal scope of protection — read this for what is actually claimed.
Technology tags used to group this patent with similar filings.
Prior art links and similar publications in this corpus.
Official abstract text for this publication.
A method for detecting a radioactive source moving on a linear path substantially parallel to an alignment of N detectors. The method includes: forming N×N t pulse counting values M i,t (i=1, 2, . . . , N and t=1, 2, . . . , N t ) from N×N t detection signals delivered by the N detectors in the form of a succession over time of N t sets of N signals simultaneously detected by the N detectors over a same duration Δt, a pulse counting value representing a number of pulses detected by a detector over a duration Δt; and computing, using a computer: a set of N t correlation products R t , a static mean R of the N×N t counting values, a correlation condition for each correlation product R t .
Opening claim text (preview).
What is claimed is: 1. A method for detecting a radioactive source moving on a linear path substantially parallel to an alignment of N detectors, N being an integer equal to or greater than 2, the method comprising: simultaneously detecting N signals by N detectors; delivering N×N t detection signals from the N detectors in the form of a succession over time of N t sets of the N signals simultaneously detected by the detector over a duration Δt, N t being significantly greater than N, a pulse counting value representing a number of pulses detected by a detector over a duration Δt; forming N×N t pulse counting values M i,t (i=1, 2, . . . , N and t=1, 2, . . . , N t ) from the N×N t detection signals; computing, using a computer: a set of N R correlation products R z so that: R z =Π i=1 N M i,[(N−i)z+1] ( z= 1,2, . . . , N R ) with N R being an integer equal to N t - 1 N - 1 , a statistical mean R of the N t products Π i=1 N M i,t such that: R _ = 1 N t ∑ t = 1 N t ∏ i = 1 N M i , t a standard deviation σ( R ) of the N t products Π i=1 N M i,t , and a correlation condition for each correlation product R z ; and determining that a radioactive source moved in front of the detectors if R z ≧ R +K 2 σ( R ), K 2 being a scalar, or determining that no radioactive source moved in front of the detectors if R z < R +K 2 σ( R ). 2. The method according to claim 1 , the method further comprising computing, by the computer, a speed V of the radioactive source as soon as a radioactive source is determined to have moved in front of the detectors, such that: V=d /( T×Δt ), where d is a distance separating two neighbouring detectors and T is a rank t of a set of N pulse counting values for which the correlation product R Z is maximum. 3. The method according to claim 1 , the method further comprising computing, by the computer, an intensity I of the radioactive source as soon as a radioactive source is determined to have moved in front of the detectors, such that: I = 1 N ∑ i = 1 N M i , ( N - i ) T + 1 - 1 N × N t ∑ t = 1 N t [ ∑ i = 1 N M i , t ] . 4. The method according to claim 1 , further comprising smoothing the pulse counting values before computing. 5. A device for detecting a radioactive source moving over a substantially linear path, the device comprising: N detectors (D i , i=1, 2, . . . , N) substantially aligned parallel to the linear path of the radioactive source, N being an integer equal to or greater than 2, the N detectors simultaneously delivering N detection signals over duration Δt, N processing circuits (T i , i=1, 2, . . . , N) connected to the N detectors, each processing circuit being configured to deliver an electronic signal corresponding to a detection signal delivered by a different detector, N counting circuits (K i , i=1, 2, . . . , N) connected to the N processing circuits, each counting circuit being configured to count, during N t successive counting durations Δt, a number of electronic pulses delivered by a diff
Physics · mapped topic
Measuring radiation intensity (G01T1/29 takes precedence {; self-powered detectors G01T3/006; using an ionisation chamber filled with a liquid or solid, e.g. frozen liquid, dielectric G01T3/008}) · CPC title
Means for conveying samples received · CPC title
Passive interrogation, i.e. by measuring radiation emitted by objects or goods · CPC title
Related publications grouped by family.
Answers are generated from the same data shown on this page.