2010
DOI: 10.1016/j.nima.2010.08.110
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High energy activation data library (HEAD-2009)

Abstract: A proton activation data library for 682 nuclides from 1 H to 210 Po in the energy range from 150 MeV up to 1 GeV was developed. To calculate proton activation data, the MCNPX 2.6.0 and CASCADE/INPE codes were chosen. Different intranuclear cascade, preequilibrium, and equilibrium nuclear reaction models and their combinations were used.The optimum calculation models have been chosen on the basis of statistical correlations for calculated and experimental proton data taken from the EXFOR library of experiment… Show more

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Cited by 21 publications
(18 citation statements)
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“…It decays with half-life 32.9 years into 42 K, a β − emitter with transition energy of 3525 keV and with a half-life of 12.36 h; high energy electrons emitted very close to the detector surface can affect the region of interest for the neutrinoless DBD of 76 Ge. Presence of 42 Ar at a higher level than expected assuming a natural abundance was observed in GERDA Phase I, which was attributed to an accumulation effect due to the attraction of the generated 42 K towards the germanium detectors. Different solutions have been considered; for the Phase II of GERDA, a nylon mini-shroud to screen the electric field of the detectors and create a barrier to avoid ion collection has been proved as an efficient method to reduce the events from 42 K; in combination with the background rejection from Pulse Shape Discrimination in BEGe detectors and LAr veto, this background is reduced by more than a factor 1000, sufficient for Phase II of the experiment [211].…”
Section: Argonmentioning
confidence: 66%
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“…It decays with half-life 32.9 years into 42 K, a β − emitter with transition energy of 3525 keV and with a half-life of 12.36 h; high energy electrons emitted very close to the detector surface can affect the region of interest for the neutrinoless DBD of 76 Ge. Presence of 42 Ar at a higher level than expected assuming a natural abundance was observed in GERDA Phase I, which was attributed to an accumulation effect due to the attraction of the generated 42 K towards the germanium detectors. Different solutions have been considered; for the Phase II of GERDA, a nylon mini-shroud to screen the electric field of the detectors and create a barrier to avoid ion collection has been proved as an efficient method to reduce the events from 42 K; in combination with the background rejection from Pulse Shape Discrimination in BEGe detectors and LAr veto, this background is reduced by more than a factor 1000, sufficient for Phase II of the experiment [211].…”
Section: Argonmentioning
confidence: 66%
“…Some of these codes have been implemented in general-purpose codes like GEANT4 [38], FLUKA [39], and MCNP [40]. Evaluated libraries of production cross sections have been elaborated, providing different coverage of reactions, projectiles, and energies, like, for example, TENDL (TALYS-based Evaluated Nuclear Data Library) [41] (based on the TALYS code, for protons and neutrons with energies up to 200 MeV) or HEAD-2009 (High Energy Activation Data) [42] (for protons and neutrons with higher energies, from 150 MeV up to 1 GeV).…”
Section: Production Cross Sectionsmentioning
confidence: 99%
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“…(1) HEAD-2009 48 cross sections have been used, if available. It is assumed that in this high energy range neutron and proton cross sections are comparable.…”
Section: Isotopementioning
confidence: 99%
“…Actinides, however, have upper limit 20 MeV. The final step is an extension to higher energies using the HEAD-2009 activation data library [31]. The HEAD-2009 library contains neutron-and protoninduced data for 684 stable and unstable nuclides from C to Po in the primary particle energy range 150 MeV to 1 GeV.…”
Section: Basic Working Principles Of Aleph2mentioning
confidence: 99%