Timing-based methods, systems, and computer readable mediums for a gated linear accelerator
US-2024100364-A1 · Mar 28, 2024 · US
US2020406063A1 · US · A1
| Field | Value |
|---|---|
| Publication number | US-2020406063-A1 |
| Application number | US-202017016372-A |
| Country | US |
| Kind code | A1 |
| Filing date | Sep 10, 2020 |
| Priority date | Apr 16, 2010 |
| Publication date | Dec 31, 2020 |
| Grant date | — |
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.
The invention comprises a method and apparatus for using a multi-layer multi-color scintillation based detector element to image a tumor of a patient using a process of determining residual energies of positively charged particles after passing through the patient, the process comprising the steps of: (1) transmitting the positively charged particles at known energies through the patient and into a multi-layer detector element; (2) detecting first and second secondary photons, resultant from passage of the positively charged particles, respectively from a first layer of a first scintillation material and a second layer of a second scintillation material at two respective layer depths, where the first wavelength range differs from the second wavelength range; (4) determining residual energies of the positively charged particles, using output from the step of detecting; and (5) relating the residual energies to body densities to generate an image.
Opening claim text (preview).
1 . An apparatus for determining residual energy of positively charged particles after passing through a patient, comprising: a multi-layer detector, comprising; a first layer comprising a first scintillation material, said first scintillation material, responsive to passage of the positively charged particles, emitting first secondary photons over a first wavelength range; and a second layer comprising a second scintillation material, said second scintillation material, responsive to passage of the positively charged particles, emitting second secondary photons over a second wavelength range, the first scintillation material differing from the second scintillation material. 2 . The apparatus of claim 1 , said multi-layer detector further comprising: a third layer comprising a third scintillation material, said third scintillation material, responsive to passage of the positively charged particles, emitting third secondary photons over a third wavelength range, said third scintillation material differing from both said first scintillation material and said second scintillation material. 3 . The apparatus of claim 2 , said multi-layer detector further comprising: a first sub-stack of scintillation materials comprising said first layer, said second layer, and said third layer; and a second sub-stack comprising a manufactured copy of said first sub-stack. 4 . The apparatus of claim 3 , said multi-layer detector further comprising: at least ten layers of scintillation materials, said at least ten layers of scintillation materials comprising: said first sub-stack; and said second sub-stack. 5 . The apparatus of claim 1 , further comprising: an imaging system configured to use output from said multi-layer detector to generate an image of a tumor of the patient. 6 . A method for determining residual energy of positively charged particles after passing through a patient, comprising the steps of: passing the positively charged particles into a multi-layer detector element; detecting first secondary photons, resultant from passage of the positively charged particles, over a first wavelength range from a first layer of said multi-layer detector, said first layer comprising a first scintillation material; and detecting second secondary photons, resultant from passage of the positively charged particles, over a second wavelength range from a second layer of said multi-layer detector element, the first wavelength range differing from the second wavelength range; accelerating the positively charged particles using an accelerator; transporting the positively charged particles from said accelerator, through the patient, and into said multi-layer detector element of a detection system; and generating an image of a tumor of the patient from output from said multi-layer detector element. 7 . The method of claim 6 , further comprising the step of: detecting third secondary photons, resultant from passage of the positively charged particles, over a third wavelength range from a third layer of said multi-layer detector element, a third mean wavelength of the third wavelength range differing from both a first mean wavelength of the first wavelength range and a second mean wavelength of the second wavelength range by at least ten nanometers.
for producing synchrotron radiation · CPC title
with immobilising means · CPC title
Transmission computed tomography [CT] · CPC title
using energy resolving detectors, e.g. photon counting · CPC title
for detecting non x-ray radiation, e.g. gamma radiation (A61B6/037 takes precedence) · CPC title
Related publications grouped by family.
Answers are generated from the same data shown on this page.