Search results for " neutron capture"

showing 10 items of 23 documents

Aza-BODIPY: A New Vector for Enhanced Theranostic Boron Neutron Capture Therapy Applications

2020

Boron neutron capture therapy (BNCT) is a radiotherapeutic modality based on the nuclear capture of slow neutrons by stable 10B atoms followed by charged particle emission that inducing extensive damage on a very localized level (&lt

Boron CompoundsBiodistributionboron compound[SDV.BIO]Life Sciences [q-bio]/BiotechnologyFluorophorein ovo modelAstrophysics::High Energy Astrophysical Phenomena[SDV]Life Sciences [q-bio]theranosticNuclear TheoryPhysics::Medical Physicsaza-BODIPY[SDV.CAN]Life Sciences [q-bio]/CancerBoron Neutron Capture Therapy010402 general chemistry01 natural sciencesSodium BorocaptateArticle03 medical and health scienceschemistry.chemical_compoundoptical imagingNIR-IMice0302 clinical medicine[SDV.CAN] Life Sciences [q-bio]/CancerPhysics::Atomic and Molecular ClustersAnimalsHumansNeutronNuclear Experiment10 B-BSHlcsh:QH301-705.5<sup>10</sup>B-BSHChemistryRadiochemistry10B-BSHGeneral MedicineFluorescence[SDV.BIO] Life Sciences [q-bio]/Biotechnology0104 chemical sciencesSWIR[SDV] Life Sciences [q-bio]Neutron capturelcsh:Biology (General)030220 oncology & carcinogenesisBNCTFemaleBODIPYEx vivoCells
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Levels of 186Re populated in thermal neutron capture reaction

2015

Levels of 186 Re have been studied in the thermal neutron capture reaction with an enriched 185 Re target. Evaluation of spectrum measured with GAMS5 allowed to obtain energies and intensities of more than 500 γ -lines assigned to 186 Re. Most of the obtained transitions have been placed in the model-independent level scheme of the doubly odd 186 Re nucleus, taking into account the available data of earlier experiments as well as the results of recent 187 Re(p, d )186 Re reaction measurements. Structure of the 186 Re low-lying levels has been analysed in terms of the particle-plus-rotor coupling model.

CouplingNuclear physicsPhysicsPhysicsQC1-999Thermal neutron captureAtomic physicsEPJ Web of Conferences
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New rotational levels in $^{186}$Re nucleus

2020

International audience; Excited levels of 186 Re have been studied using results of the single γ -ray spectra measurements following the thermal neutron capture reaction. Energies and intensities of more than 500 γ -transitions have been obtained with the high-resolution crystal diffraction spectrometer GAMS5 of ILL. Most of the obtained intense γ -transitions have been placed in the 186 Re level scheme. A number of new levels, as well as the depopulation for levels observed earlier in the 187 Re (p,d)186 Re reaction measurements have been proposed. Structure of 186 Re levels is interpreted in terms of two-quasiparticle plus rotor coupling model and compared with that of the neighbouring do…

DiffractionNuclear and High Energy PhysicsCore plus two-quasiparticles model[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]Thermal neutron captureNUCLEAR REACTION 185Re[formula omitted]E=thermalMeasured [formula omitted]01 natural sciencesSpectral lineCrystalMeasured Eγ0103 physical sciencesmedicineγ)010306 general physicsPhysicsCouplingSpectrometer010308 nuclear & particles physics186 Re deduced levelsNUCLEAR REACTION 185 Re (nmedicine.anatomical_structureE =thermalExcited stateGAMS5 crystal diffraction spectrometerAtomic physicsNucleus186Re deduced levels
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Dose determination using alanine detectors in a mixed neutron and gamma field for boron neutron capture therapy of liver malignancies

2011

IntroductionBoron Neutron Capture Therapy for liver malignancies is being investigated at the University of Mainz. One important aim is the set-up of a reliable dosimetry system. Alanine dosimeters have previously been applied for dosimetry of mixed radiation fields in antiproton therapy, and may be suitable for measurements in mixed neutron and gamma fields.Materials and MethodsTwo experiments have been carried out in the thermal column of the TRIGA Mark II reactor at the University of Mainz. Alanine dosimeters have been irradiated in a phantom and in liver tissue.ResultsFor the interpretation and prediction of the dose for each pellet, beside the results of the measurements, calculations …

Monte Carlo methodBoron Neutron Capture TherapyImaging phantomTRIGAIonizing radiationRadiation MonitoringHumansMedicineDosimetryRadiology Nuclear Medicine and imagingNeutronRadiometryNeutronsAlanineDosimeterPhantoms Imagingbusiness.industryLiver NeoplasmsRadiochemistryDose-Response Relationship RadiationHematologyGeneral MedicineNeutron captureLiverOncologyGamma RaysbusinessNuclear medicineMonte Carlo MethodActa Oncologica
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GEANT4 simulation of the neutron background of the C6D6 set-up for capture studies at n_TOF

2014

The neutron sensitivity of the C6D6 detector setup used at n_TOF facility for capture measurements has been studied by means of detailed GEANT4 simulations. A realistic software replica of the entire n_TOF experimental hall, including the neutron beam line, sample, detector supports and the walls of the experimental area has beeni mplemented in the simulations. The simulations have been analyzed in the same manner as experimental data, in particular by applying the Pulse Height Weighting Technique. The simulations have been validated against a measurement of the neutron background performed with anatC sample, showing an excellent agreement above 1 keV. At lower energies, an additional compo…

Neutron captureNuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaGEANT4 simulations; Neutron time of flight; Neutron background; n_TOF; Neutron captureFOS: Physical sciencesNeutronN-TOF7. Clean energy01 natural sciencesPartícules (Física nuclear)Nuclear physicsCross section (physics)0103 physical sciencesNeutronNuclear Experiment (nucl-ex)010306 general physicsGEANT4 simulations;N-TOF;Neutron time of flight;Neutron capture;Neutron backgroundNuclear ExperimentInstrumentationphysics.ins-detNuclear ExperimentGEANT4Line (formation)Particles (Nuclear physics)PhysicsBonner sphere:Energies::Energia nuclear [Àrees temàtiques de la UPC]NeutronsGEANT4 simulation:Física [Àrees temàtiques de la UPC]010308 nuclear & particles physicsDetectorFísicaNeutron sensitivityDetectorInstrumentation and Detectors (physics.ins-det)Neutron radiationNEUTRON TIME OF FLIGHTNeutron captureBackgroundDeuteriumN_TOFGEANT4 simulationsNeutron backgroundSimulation
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Experimental neutron capture data of 58Ni from the CERN n_TOF facility

2014

The $^{58}$Ni $(n,\gamma)$ cross section has been measured at the neutron time of flight facility n_TOF at CERN, in the energy range from 27 meV up to 400 keV. In total, 51 resonances have been analyzed up to 122 keV. Maxwellian averaged cross sections (MACS) have been calculated for stellar temperatures of kT$=$5-100 keV with uncertainties of less than 6%, showing fair agreement with recent experimental and evaluated data up to kT = 50 keV. The MACS extracted in the present work at 30 keV is 34.2$\pm$0.6$_\mathrm{stat}\pm$1.8$_\mathrm{sys}$ mb, in agreement with latest results and evaluations, but 12% lower relative to the recent KADoNIS compilation of astrophysical cross sections. When in…

Nuclear and High Energy PhysicsnTOFAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciencesNEUTRON RESONANCE ANALYSISNeutron[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesNuclear physicsTime of flight58Ni neutron capture cross section; n_TOF; MACS0103 physical sciencesNeutron cross section:Física::Electromagnetisme [Àrees temàtiques de la UPC]Nuclear Physics - ExperimentNeutronNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentPhysicsNeutronsLarge Hadron ColliderCross section010308 nuclear & particles physicsCERN - n_TOFResonanceFísicaNEUTRON TIME OF FLIGHTNeutron temperatureTime of flightNeutron captureNeutrons CaptureS PROCESSs-process
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New measurement of the 242Pu(n,γ) cross section at n-TOF-EAR1 for MOX fuels: Preliminary results in the RRR

2016

The spent fuel of current nuclear reactors contains fissile plutonium isotopes that can be combined with 238U to make mixed oxide (MOX) fuel. In this way the Pu from spent fuel is used in a new reactor cycle, contributing to the long-term sustainability of nuclear energy. The use of MOX fuels in thermal and fast reactors requires accurate capture and fission cross sections. For the particular case of 242Pu, the previous neutron capture cross section measurements were made in the 70’s, providing an uncertainty of about 35% in the keV region. In this context, the Nuclear Energy Agency recommends in its “High Priority Request List” and its report WPEC-26 that the capture cross section of 242Pu…

Nuclear reactionnTOFQC1-999Nuclear engineeringContext (language use)CERN nTOFNeutron[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences7. Clean energyPhysics and Astronomy (all)Nuclear reactorsReactors nuclears0103 physical sciencesCERNNeutron cross sectionNuclear Physics - ExperimentNeutronddc:530242Pu neutron capture010306 general physicsMOX fuelNeutrons:Energies::Energia nuclear [Àrees temàtiques de la UPC]Fissile materialCross section:Física [Àrees temàtiques de la UPC]010308 nuclear & particles physicsPhysicsNuclear reactionSpent nuclear fuelNeutron temperature13. Climate actionneutron time-of-flight measurement
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The FiR 1 photon beam model adjustment according to in-air spectrum measurements with the Mg(Ar) ionization chamber.

2014

Abstract The mixed neutron–photon beam of FiR 1 reactor is used for boron–neutron capture therapy (BNCT) in Finland. A beam model has been defined for patient treatment planning and dosimetric calculations. The neutron beam model has been validated with an activation foil measurements. The photon beam model has not been thoroughly validated against measurements, due to the fact that the beam photon dose rate is low, at most only 2% of the total weighted patient dose at FiR 1. However, improvement of the photon dose detection accuracy is worthwhile, since the beam photon dose is of concern in the beam dosimetry. In this study, we have performed ionization chamber measurements with multiple b…

PhotonQuantitative Biology::Tissues and OrgansPhysics::Medical PhysicsMonte Carlo methodAnalytical chemistryBoron Neutron Capture TherapySensitivity and SpecificityOpticsNuclear ReactorsDosimetryPenelopeIonization ChamberDosimetryComputer SimulationPhoton beamRadiometryMonte CarloPhysicsPhotonsRadiationModels Statisticalbusiness.industryAirRadiotherapy Planning Computer-AssistedReproducibility of ResultsEquipment DesignNeutron radiationEquipment Failure AnalysisIonization chamberBNCTPhysics::Accelerator PhysicsComputer-Aided DesignDose ratebusinessMCNP5Beam (structure)Applied radiation and isotopes : including data, instrumentation and methods for use in agriculture, industry and medicine
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Gamma Ray Spectra from Thermal Neutron Capture on Gadolinium-155 and Natural Gadolinium

2019

Natural gadolinium is widely used for its excellent thermal neutron capture cross section, because of its two major isotopes: $^{\rm 155}$Gd and $^{\rm 157}$Gd. We measured the $\gamma$-ray spectra produced from the thermal neutron capture on targets comprising a natural gadolinium film and enriched $^{\rm 155}$Gd (in Gd$_{2}$O$_{3}$ powder) in the energy range from 0.11 MeV to 8.0 MeV, using the ANNRI germanium spectrometer at MLF, J-PARC. The freshly analysed data of the $^{\rm 155}$Gd(n, $\gamma$) reaction are used to improve our previously developed model (ANNRI-Gd model) for the $^{\rm 157}$Gd(n, $\gamma$) reaction, and its performance confirmed with the independent data from the $^{\r…

Physics - Instrumentation and DetectorsGadoliniumMonte Carlo methodAnalytical chemistryenergy spectrumGeneral Physics and Astronomychemistry.chemical_elementFOS: Physical sciencesGermanium[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]n: thermal7. Clean energy01 natural sciencesSpectral lineHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)F20 Instrumentation and technique0103 physical sciencesH43 Software architectures[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex][PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Nuclear Experiment (nucl-ex)n: capture010306 general physicsNuclear ExperimentMonte CarloPhysicsD21 Models of nuclear reactionsIsotopeSpectrometer010308 nuclear & particles physicsJ-PARC LabGamma rayInstrumentation and Detectors (physics.ins-det)Gadolinium neutron capture gamma ray cascadeNeutron temperature3. Good healthparticle: interactionH20 Instrumentation for underground experimentsgermaniumF22 Neutrinos from supernova remnant and other astronomical objectsC42 Reactor experimentschemistrygamma rayC43 Underground experimentsspectrometergadoliniumperformance
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Measurement of the Pu-242(n,gamma) cross section from thermal to 500 keV at the Budapest research reactor and CERN n_TOF-EAR1 facilities

2019

The design and operation of innovative nuclear systems requires a better knowledge of the capture and fission cross sections of the Pu isotopes. For the case of capture on 242Pu, a reduction of the uncertainty in the fast region down to 8-12% is required. Moreover, aiming at improving the evaluation of the fast energy range in terms of average parameters, the OECD NEA High Priority Request List (HPRL) requests high-resolution capture measurements with improved accuracy below 2 keV. The current uncertainties also affect the thermal point, where previous experiments deviate from each other by 20%. A fruitful collaboration betwen JGU Mainz and HZ Dresden-Rossendorf within the EC CHANDA project…

PhysicsLarge Hadron ColliderIsotope010308 nuclear & particles physicsFissionPhysicsQC1-999n_TOF 242Pu neutron capture neutron time of flight[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences7. Clean energyResonance (particle physics)Nuclear physicsStack (abstract data type)0103 physical sciencesNeutronResearch reactorNuclear Physics - ExperimentNeutron activation analysis010306 general physics
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