FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W2940980201> ?p ?o ?g. }

• W2940980201 endingPage "2743" @default.
• W2940980201 startingPage "2735" @default.
• W2940980201 abstract "X-ray fluorescence CT (XFCT) has shown promise for molecular imaging of gold nanoparticles. To date, XFCT has been induced by kilovoltage photon beams due to the high photoelectric interaction probability. We compare K-shell and L-shell XFCT induced by photon, electron, and proton beams for two phantom sizes. A 2.5 and 5.0-cm diameter phantom with four 5 mm and 10 mm vials, respectively, with gold-solutions of 0.1%-2% by weight were built in TOPAS, a GEANT4-based Monte Carlo simulation tool. The 2.5-cm phantom was imaged with XFCT induced by beams of 7.45×104 81 keV- and 5 MeV-photons, 220 kVp- and 6 MV-photons, 10 MeV- and 100 MeV-electrons, and 100 MeV- and 250 MeV-protons. The doses between each phantom size were equal. First-generation CT geometry with 0.5 mm × 0.5 mm pencil beams with 0.5 mm-translation and 2°-rotation steps over each phantom was modeled. The scattered x-rays were detected on an idealized spherical detector from which the K-shell and L-shell fluorescent x-rays were extracted in 0.5 keV and 0.2 keV bins. XFCT images were generated using iterative reconstruction algorithms. The highest gold sensitivity was seen in the 81 keV-photon K-shell and L-shell images (0.004% and 0.007%) of the 5.0 cm-phantom at 30 mGy. For the 2.5 cm-phantom, the detection limits were 0.006%, 0.62%, and 0.28% for 81 keV-photon K-shell, 100 MeV-electron K-shell, and 100 MeV-proton L-shell images, respectively. The mean imaging dose was approximately 2-3 orders of magnitude higher in electron- and proton-XFCT compared to 81keV-photon XFCT. Our MC study demonstrates that the small-object XFCT imaging achieves the best performance when induced with kilovoltage-photon beams. Due to high imaging doses, electron- and proton-induced XFCT might be feasible for guiding nanoparticle-enhanced charged-particle radiotherapy." @default.
• W2940980201 created "2019-05-03" @default.
• W2940980201 creator A5022479825 @default.
• W2940980201 creator A5051694808 @default.
• W2940980201 date "2019-12-01" @default.
• W2940980201 modified "2023-09-28" @default.
• W2940980201 title "X-Ray Fluorescence Computed Tomography Induced by Photon, Electron, and Proton Beams" @default.
• W2940980201 cites W1753081326 @default.
• W2940980201 cites W1912693941 @default.
• W2940980201 cites W1978153144 @default.
• W2940980201 cites W1981418870 @default.
• W2940980201 cites W2001122017 @default.
• W2940980201 cites W2029532403 @default.
• W2940980201 cites W2030544564 @default.
• W2940980201 cites W2031864052 @default.
• W2940980201 cites W2039075972 @default.
• W2940980201 cites W2046031025 @default.
• W2940980201 cites W2051584429 @default.
• W2940980201 cites W2061294304 @default.
• W2940980201 cites W2069629287 @default.
• W2940980201 cites W2069851326 @default.
• W2940980201 cites W2072180179 @default.
• W2940980201 cites W2110721989 @default.
• W2940980201 cites W2128158076 @default.
• W2940980201 cites W2135396471 @default.
• W2940980201 cites W2145238798 @default.
• W2940980201 cites W2795111039 @default.
• W2940980201 cites W2804370793 @default.
• W2940980201 cites W2898776965 @default.
• W2940980201 cites W4254693803 @default.
• W2940980201 doi "https://doi.org/10.1109/tmi.2019.2912137" @default.
• W2940980201 hasPubMedId "https://pubmed.ncbi.nlm.nih.gov/31021762" @default.
• W2940980201 hasPublicationYear "2019" @default.
• W2940980201 type Work @default.
• W2940980201 sameAs 2940980201 @default.
• W2940980201 citedByCount "2" @default.
• W2940980201 countsByYear W29409802012022 @default.
• W2940980201 countsByYear W29409802012023 @default.
• W2940980201 crossrefType "journal-article" @default.
• W2940980201 hasAuthorship W2940980201A5022479825 @default.
• W2940980201 hasAuthorship W2940980201A5051694808 @default.
• W2940980201 hasConcept C104293457 @default.
• W2940980201 hasConcept C105795698 @default.
• W2940980201 hasConcept C120665830 @default.
• W2940980201 hasConcept C121332964 @default.
• W2940980201 hasConcept C147120987 @default.
• W2940980201 hasConcept C159317903 @default.
• W2940980201 hasConcept C185544564 @default.
• W2940980201 hasConcept C19499675 @default.
• W2940980201 hasConcept C33923547 @default.
• W2940980201 hasConcept C54516573 @default.
• W2940980201 hasConceptScore W2940980201C104293457 @default.
• W2940980201 hasConceptScore W2940980201C105795698 @default.
• W2940980201 hasConceptScore W2940980201C120665830 @default.
• W2940980201 hasConceptScore W2940980201C121332964 @default.
• W2940980201 hasConceptScore W2940980201C147120987 @default.
• W2940980201 hasConceptScore W2940980201C159317903 @default.
• W2940980201 hasConceptScore W2940980201C185544564 @default.
• W2940980201 hasConceptScore W2940980201C19499675 @default.
• W2940980201 hasConceptScore W2940980201C33923547 @default.
• W2940980201 hasConceptScore W2940980201C54516573 @default.
• W2940980201 hasIssue "12" @default.
• W2940980201 hasLocation W29409802011 @default.
• W2940980201 hasLocation W29409802012 @default.
• W2940980201 hasOpenAccess W2940980201 @default.
• W2940980201 hasPrimaryLocation W29409802011 @default.
• W2940980201 hasRelatedWork W1981117618 @default.
• W2940980201 hasRelatedWork W2065540975 @default.
• W2940980201 hasRelatedWork W2096009385 @default.
• W2940980201 hasRelatedWork W2505685125 @default.
• W2940980201 hasRelatedWork W2601785848 @default.
• W2940980201 hasRelatedWork W3151437434 @default.
• W2940980201 hasRelatedWork W4313255511 @default.
• W2940980201 hasRelatedWork W4313537251 @default.
• W2940980201 hasRelatedWork W901888691 @default.
• W2940980201 hasRelatedWork W2015920351 @default.
• W2940980201 hasVolume "38" @default.
• W2940980201 isParatext "false" @default.
• W2940980201 isRetracted "false" @default.
• W2940980201 magId "2940980201" @default.
• W2940980201 workType "article" @default.