Kluge et al., 2019 - Google Patents
Optimization and characterization of the PGAI-NT instrument's Neutron Tomography set-up at MLZKluge et al., 2019
- Document ID
- 235798957821201677
- Author
- Kluge E
- Stieghorst C
- Révay Z
- Kudějová P
- Jolie J
- Publication year
- Publication venue
- Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
External Links
Snippet
Abstract The Prompt Gamma-ray Activation Imaging and Neutron Tomography (PGAI-NT) instrument at the PGAA facility of the Heinz Maier-Leibnitz Center (MLZ), provides a method to obtain and effectively visualize position-sensitive element abundances in samples by …
- 238000003325 tomography 0 title abstract description 33
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01T—MEASUREMENT OF NUCLEAR OR X-RADIATION
- G01T1/00—Measuring X-radiation, gamma radiation, corpuscular radiation, or cosmic radiation
- G01T1/16—Measuring radiation intensity
- G01T1/161—Application in the field of nuclear medicine, e.g. in vivo counting
- G01T1/164—Scintigraphy
- G01T1/1641—Static instruments for imaging the distribution of radioactivity in one or two dimensions using one or several scintillating elements; Radio-isotope cameras
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01T—MEASUREMENT OF NUCLEAR OR X-RADIATION
- G01T1/00—Measuring X-radiation, gamma radiation, corpuscular radiation, or cosmic radiation
- G01T1/29—Measurement performed on radiation beams, e.g. position or section of the beam; Measurement of spatial distribution of radiation
- G01T1/2914—Measurement of spatial distribution of radiation
- G01T1/2985—In depth localisation, e.g. using positron emitters; Tomographic imaging (longitudinal and transverse section imaging; apparatus for radiation diagnosis sequentially in different planes, steroscopic radiation diagnosis)
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N23/00—Investigating or analysing materials by the use of wave or particle radiation not covered by G01N21/00 or G01N22/00, e.g. X-rays or neutrons
- G01N23/02—Investigating or analysing materials by the use of wave or particle radiation not covered by G01N21/00 or G01N22/00, e.g. X-rays or neutrons by transmitting the radiation through the material
- G01N23/04—Investigating or analysing materials by the use of wave or particle radiation not covered by G01N21/00 or G01N22/00, e.g. X-rays or neutrons by transmitting the radiation through the material and forming a picture
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N2223/00—Investigating materials by wave or particle radiation
- G01N2223/07—Investigating materials by wave or particle radiation secondary emission
- G01N2223/076—X-ray fluorescence
-
- G—PHYSICS
- G21—NUCLEAR PHYSICS; NUCLEAR ENGINEERING
- G21K—TECHNIQUES FOR HANDLING PARTICLES OR IONISING RADIATION NOT OTHERWISE PROVIDED FOR; IRRADIATION DEVICES; GAMMA RAY OR X-RAY MICROSCOPES
- G21K1/00—Arrangements for handling particles or ionizing radiation, e.g. focusing or moderating
- G21K1/02—Arrangements for handling particles or ionizing radiation, e.g. focusing or moderating using diaphragms, collimators
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N23/00—Investigating or analysing materials by the use of wave or particle radiation not covered by G01N21/00 or G01N22/00, e.g. X-rays or neutrons
- G01N23/20—Investigating or analysing materials by the use of wave or particle radiation not covered by G01N21/00 or G01N22/00, e.g. X-rays or neutrons by using diffraction of the radiation, e.g. for investigating crystal structure; by using reflection of the radiation
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N2223/00—Investigating materials by wave or particle radiation
- G01N2223/60—Specific applications or type of materials
-
- G—PHYSICS
- G21—NUCLEAR PHYSICS; NUCLEAR ENGINEERING
- G21G—CONVERSION OF CHEMICAL ELEMENTS; RADIOACTIVE SOURCES
- G21G1/00—Arrangements for converting chemical elements by electromagnetic radiation, corpuscular radiation or particle bombardment, e.g. producing radioactive isotopes
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| Verburg et al. | Proton range verification through prompt gamma-ray spectroscopy | |
| Fontana et al. | Compton camera study for high efficiency SPECT and benchmark with Anger system | |
| Battistoni et al. | The FLUKA code: an accurate simulation tool for particle therapy | |
| Kelleter et al. | Spectroscopic study of prompt-gamma emission for range verification in proton therapy | |
| Yamaguchi et al. | Imaging of monochromatic beams by measuring secondary electron bremsstrahlung for carbon-ion therapy using a pinhole x-ray camera | |
| EP2977083B1 (en) | An apparatus for particle therapy verification | |
| RU2598396C2 (en) | Method and system of combined radiation nondestructive control | |
| Kis et al. | NIPS–NORMA station—A combined facility for neutron-based nondestructive element analysis and imaging at the Budapest Neutron Centre | |
| Shao et al. | In-beam PET imaging for on-line adaptive proton therapy: an initial phantom study | |
| Ando et al. | Development of a low-energy x-ray camera for the imaging of secondary electron bremsstrahlung x-ray emitted during proton irradiation for range estimation | |
| Chuong et al. | Validation of gamma scanning method for optimizing NaI (Tl) detector model in Monte Carlo simulation | |
| Ahmed et al. | A Monte Carlo model of a benchtop X-ray fluorescence computed tomography system and its application to validate a deconvolution-based X-ray fluorescence signal extraction method | |
| Craft et al. | Characterization of a neutron beam following reconfiguration of the Neutron Radiography Reactor (NRAD) core and addition of new fuel elements | |
| Thanh et al. | A prototype of radioactive waste drum monitor by non-destructive assays using gamma spectrometry | |
| Lopes et al. | Simulation of proton range monitoring in an anthropomorphic phantom using multi-slat collimators and time-of-flight detection of prompt-gamma quanta | |
| Cho et al. | Energy response calibration of photon-counting detectors using x-ray fluorescence: a feasibility study | |
| Kluge et al. | Optimization and characterization of the PGAI-NT instrument’s Neutron Tomography set-up at MLZ | |
| Morris et al. | Qualitative comparison of bremsstrahlung x-rays and 800 MeV protons for tomography of urania fuel pellets | |
| Barrientos et al. | Gamma-ray sources imaging and test-beam results with MACACO III Compton camera | |
| Johnson | Meeting the detector challenges for pre-clinical proton and ion computed tomography | |
| Gutierrez et al. | Progress towards a semiconductor Compton camera for prompt gamma imaging during proton beam therapy for range and dose verification | |
| Parajuli et al. | Carbon range verification with 718 keV Compton imaging | |
| Dyussambayev et al. | TITAN neutron imaging facility performance | |
| Kouwenberg et al. | Alpha radiation dosimetry using fluorescent nuclear track detectors | |
| Hosobuchi et al. | Demonstrative measurement of proton-nuclear reaction by deconvolving the prompt gamma-ray spectra |