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dc.creatorAlcayne, V.es
dc.creatorCano-Ott, D.es
dc.creatorGarcia, J.es
dc.creatorGonzález-Romero, E.es
dc.creatorMartínez, T.es
dc.creatorMendoza, E.es
dc.creatorSánchez, A.es
dc.creatorPlaza, J.es
dc.creatorBalibrea-Correa, J.es
dc.creatorCasanovas, A.es
dc.creatorDomingo-Pardo, C.es
dc.creatorLerendegui Marco, Jorgees
dc.creatorCortés Giraldo, Miguel Antonioes
dc.creatorPérez Maroto, Pabloes
dc.creatorQuesada Molina, José Manueles
dc.creatorZugec, P.es
dc.creatorn_TOF Collaboration (Autoría grupal)es
dc.date.accessioned2024-05-20T16:49:24Z
dc.date.available2024-05-20T16:49:24Z
dc.date.issued2023
dc.identifier.citationAlcayne, V., Cano-Ott, D., Garcia, J., González-Romero, E., Martínez, T., Mendoza, E.,...,n_TOF Collaboration (Autoría grupal), (2023). A segmented total energy detector (sTED) for (n, gamma) cross section measurements at n_TOF EAR2. En 15th International Conference on Nuclear Data for Science and Technology (ND2022) (01043-), EPJ Web of Conf..
dc.identifier.issn2100-014Xes
dc.identifier.urihttps://hdl.handle.net/11441/158703
dc.description.abstractThe neutron time-of-flight facility n_TOF is characterised by its high instantaneous neutron intensity, high resolution and broad neutron energy spectra, specially conceived for neutron-induced reaction cross section measurements. Two Time-Of-Flight (TOR) experimental areas are available at the facility: experimental area 1 (EAR1), located at the end of the 185 m horizontal flight path from the spallation target, and experimental area 2 (EAR2), placed at 20 m from the target in the vertical direction. The neutron fluence in EAR2 is similar to 300 times more intense than in EARL in the relevant time-of-flight window. EAR2 was designed to carry out challenging cross-section measurements with low mass samples (approximately 1 mg), reactions with small cross-sections or/and highly radioactive samples. The high instantaneous fluence of EAR2 results in high counting rates that challenge the existing capture systems. Therefore, the sTED detector has been designed to mitigate these effects. In 2021, a dedicated campaign was done validating the performance of the detector up to at least 300 keV neutron energy. After this campaign, the detector has been used to perform various capture cross section measurements at n_TOF EAR2.es
dc.description.sponsorshipMinisterio de Ciencia e Innovación PGC2018-096717-B-C21es
dc.description.sponsorshipEuropean Commision 847552es
dc.formatapplication/pdfes
dc.format.extent5 p.es
dc.language.isoenges
dc.publisherEPJ Web of Conf.es
dc.relation.ispartof15th International Conference on Nuclear Data for Science and Technology (ND2022) (2023), pp. 01043-..
dc.rightsAtribución 4.0 Internacional*
dc.rights.urihttp://creativecommons.org/licenses/by/4.0/*
dc.titleA segmented total energy detector (sTED) for (n, gamma) cross section measurements at n_TOF EAR2es
dc.typeinfo:eu-repo/semantics/conferenceObjectes
dc.type.versioninfo:eu-repo/semantics/publishedVersiones
dc.rights.accessRightsinfo:eu-repo/semantics/openAccesses
dc.contributor.affiliationUniversidad de Sevilla. Departamento de Física Atómica, Molecular y Nucleares
dc.relation.projectIDPGC2018-096717-B-C21es
dc.relation.projectID847552es
dc.relation.publisherversionhttps://doi.org/10.1051/epjconf/202328401043es
dc.identifier.doi10.1051/epjconf/202328401043es
dc.publication.initialPage01043es
dc.eventtitle15th International Conference on Nuclear Data for Science and Technology (ND2022)es
dc.contributor.funderMinisterio de Ciencia e Innovación (MICIN). Españaes
dc.contributor.funderEuropean Commission (EC)es

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