Method and apparatus for capturing volume information of three-dimensional samples
US-11215536-B2 · Jan 4, 2022 · US
US11614552B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-11614552-B2 |
| Application number | US-202016853520-A |
| Country | US |
| Kind code | B2 |
| Filing date | Apr 20, 2020 |
| Priority date | Apr 18, 2019 |
| Publication date | Mar 28, 2023 |
| Grant date | Mar 28, 2023 |
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 volume interrogation system can use an accelerated beam of charged particles to interrogate objects using charged-particle attenuation and scattering tomography to screen items such as portable electronic devices, packages, baggage, industrial products, or food products for the presence of materials of interest inside. The exemplary systems and methods in this patent document can be employed in checkpoint applications to scan items. Such checkpoint applications can include border crossings, mass transit terminals (subways, buses, railways, ferries, etc.), and government and private-sector facilities.
Opening claim text (preview).
What is claimed is: 1. A scanner for interrogating contents of a volume comprising: an accelerator structured to generate a beam of charged particles; a chamber located in a path of the beam of charged particles to receive the beam of charged particles; a beam steering system located in the chamber to receive the beam of charged particles and structured to scan the beam of charged particles over a range of beam angles; a translation stage located in a path of the scanned beam of charged particles from the beam steering system, the translation stage is configured to support an object to be scanned, and the translation stage is operable to move the object relative to the scanned beam of charged particles; a first particle tracking detector located above the translation stage to receive charged particles that transit through the object and to measure position and direction of the charged particles that transit through the object while allowing the charged particles to pass through; a second particle tracking detector located below the translation stage and opposite to the first particle tracking detector, wherein the second particle tracking detector structured to receive and measure position and direction of the charged particles before the charged particles transit though the object while allowing the charged particles to pass through; a calorimeter located above the first particle tracking detector to receive the charged particles from the first particle tracking detector and to measure the received charged particles to represent energy of the charged particles received by the first particle tracking detector; and a processor communicably coupled to the first particle tracking detector, the second particle tracking detector, and the calorimeter, wherein the processor is configured to: calculate scattering angles of the charged particles by measuring trajectories of the charged particles before the charged particles enter the object and after the charged particles exit the object, wherein the scattering angles are calculated using data provided by the first particle tracking detector and the second particle tracking detector; determine energy loss of the charged particles based on energy related data provided by the calorimeter related to the energy of the charged particles received by the first particle tracking detector, wherein the energy loss is determined by the processor configured to subtract the energy of the charged particles received by the first particle tracking detector from a pre-determined energy associated with the charged particles generated by the accelerator; obtain an estimate of a spatial map of atomic number and density of the object based on the scattering angles and the energy loss. 2. The scanner of claim 1 , wherein the beam steering system comprises: a primary steering magnet structured to receive the beam of charged particles from the accelerator, wherein the primary steering magnet is enabled to laterally sweep the beam; two wedge magnets structured to receive the laterally swept beam and to direct charged particles in a vertical trajectory so that the beam is rastered in position; and a secondary steering magnet structured to receive the rastered beam and to adjust angles of the charged particles that arrive at the object. 3. The scanner of claim 2 , wherein the beam steering system further comprises: a bend magnet located in between the accelerator and the primary steering magnet, wherein the bend magnet is structured to receive the charged particles from the accelerator, and wherein the bend magnet is structured to orient the charged particles toward the primary steering magnet. 4. The scanner of claim 3 , further comprising: a collimator located between the bend magnet and the primary steering magnet, wherein the collimator is structured to receive the charged particles from the bend magnet and to direct the charged particles towards the primary steering magnet, and wherein the collimator is structured to absorb any stray charged particles. 5. The scanner of claim 2 , wherein the beam steering system further comprises: one or more electromagnets enabled to provide trim fields to correct imperfections in a field of the two wedge magnets or to compensate for variations in beam energy. 6. The scanner of claim 2 , wherein the two wedge magnets are electro-magnets. 7. The scanner of claim 1 , wherein the first particle tracking detector comprises two or more layers of charged particle detectors with each layer being perpendicular to at least one other layer and each layer including a plurality of charged particle detectors parallel to each other and structured to convert deposited energy from at least some of the charged particles into electrical current. 8. The scanner of claim 7 , wherein the charged particle detectors comprise scintillating fibers coupled with silicon photomultiplier sensors. 9. The scanner of claim 1 , wherein the second particle tracking detector comprises two or more layers of charged particle detectors with each layer being perpendicular to at least one other layer and each layer including a plurality of charged particle detectors parallel to each other and structured to convert deposited energy from at least some of the charged particles into electrical current. 10. The scanner of claim 9 , wherein the charged particle detectors comprise scintillating fibers coupled to silicon photomultiplier sensors. 11. The scanner of claim 1 , wherein the calorimeter comprises: a first type of scintillator encased in a light box and structured to convert energy of the charged particles into optical photons and to stop the charged particles to minimize X-ray generation, wherein the light box includes an orifice that corresponds to an opening in the calorimeter to receive the charged particles; and one or more photomultiplier tubes coupled to the light box and structured to detect the optical photons. 12. The scanner of claim 11 , wherein the first type of scintillator comprises a single crystal stilbene. 13. The scanner of claim 11 , wherein the first type of scintillator is wrapped in an optical reflecting material. 14. The scanner of claim 11 , wherein the calorimeter further comprises: a second type of scintillator surrounding the first type of scintillator and encased in the light box, the second type of scintillator structured to convert energy of the charged particles into optical photons and to capture X-rays generated from the charged particles. 15. The scanner of claim 14 , wherein the second type of scintillator comprises lead tungstate. 16. The scanner of claim 14 , wherein the second type of scintillator is wrapped in an optical reflecting material. 17. The scanner of claim 1 , wherein the translation stage is a conveyor belt. 18. The scanner of claim 1 , wherein the charged particles include electrons. 19. The scanner of claim 1 , wherein the beam steering system is kept under a vacuum condition in the chamber. 20. A scanner for interrogating contents of a volume comprising: an accelerator structured to generate a beam of charged particles; a chamber located in a path of the beam of charged particles to receive the beam of charged particles; a beam steering system located in the chamber to receive the beam of charged particles and structured to scan the beam of charged particles over a range of beam angles, wherein the beam steering system comprises: a primary steering magnet structured to receive the beam of charged particles from th
Arrangements for beam delivery or irradiation (irradiation systems per se G21K5/00) · CPC title
Scintillation chambers (discharge tubes H01J40/00, H01J47/00) · CPC title
for beam bending · CPC title
Magnetic resonance accelerators; Cyclotrons {(strophotrons, turbine tubes H01J25/62)} · CPC title
Magnet systems {, e.g. undulators, wigglers (free-electron laser H01S3/0903)}; Energisation thereof · CPC title
Related publications grouped by family.
Answers are generated from the same data shown on this page.