Distribution of neutrons and protons in elongated targets

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dc.contributor.authorZeman, Miroslavcs
dc.contributor.authorAdam, Jindřichcs
dc.contributor.authorBaldin, Anton Alexandrovichcs
dc.contributor.authorBrunčiaková, Miriamacs
dc.contributor.authorGustov, S.A.cs
dc.contributor.authorKatovský, Karelcs
dc.contributor.authorKhushvaktov, Jurabekcs
dc.contributor.authorKrál, Dušancs
dc.contributor.authorSolnyshkin, Alexander A.cs
dc.contributor.authorSvoboda, Josefcs
dc.contributor.authorŠťastný, Ondřejcs
dc.contributor.authorTichý, Pavelcs
dc.contributor.authorTyutyunnikov, S.cs
dc.contributor.authorVrzalová, Jitkacs
dc.contributor.authorWagner, Vladimírcs
dc.contributor.authorZávorka, Lukášcs
dc.coverage.issue1cs
dc.coverage.volume239cs
dc.date.issued2020-10-03cs
dc.description.abstractAnalysis of neutron distribution was carried out for two elongated targets. The targets have cylindrical shape and are made of lead and carbon, respectively. The dimensions are approximately one meter in length and 19 cm in diameter. The targets were irradiated with 660 MeV proton beam at Phasotron accelerator at the Joint Institute for Nuclear Research. The total number of protons was 2.35(18)E15 for the experiment with carbon target and the total number of particles at the second experiment was 2.32(19)E15. The produced neutron field was monitored by cobalt threshold activation detectors at various positions. The activation detectors were measured by means of gamma spectroscopy using HPGe detectors. Reaction rates of different radionuclides produced in the activation detectors were determined and the results from both experiments were compared. The ratios were calculated for 7 reactions produced in cobalt detectors. The ratio of the reaction rates shows that the number of residual nuclei with higher threshold energies is higher for experiment with carbon target than for the experiment with the lead target.en
dc.formattextcs
dc.format.extent1-4cs
dc.format.mimetypeapplication/pdfcs
dc.identifier.citationEPJ Web of Conferences. 2020, vol. 239, issue 1, p. 1-4.en
dc.identifier.doi10.1051/epjconf/202023906005cs
dc.identifier.isbn978-2-7598-9106-1cs
dc.identifier.issn2100-014Xcs
dc.identifier.orcid0000-0003-3502-6684cs
dc.identifier.orcid0000-0002-9850-7007cs
dc.identifier.orcid0000-0001-9335-8199cs
dc.identifier.orcid0000-0001-5865-7273cs
dc.identifier.orcid0000-0003-0614-7954cs
dc.identifier.orcid0000-0002-0451-7977cs
dc.identifier.other166128cs
dc.identifier.researcheridO-6229-2018cs
dc.identifier.researcheridK-2656-2016cs
dc.identifier.researcheridU-7790-2017cs
dc.identifier.researcheridAAO-7124-2021cs
dc.identifier.researcheridQ-8955-2017cs
dc.identifier.scopus6507230729cs
dc.identifier.scopus57203038812cs
dc.identifier.scopus57191078125cs
dc.identifier.urihttp://hdl.handle.net/11012/201674
dc.language.isoencs
dc.publisherEDP Sciencescs
dc.relation.ispartofEPJ Web of Conferencescs
dc.relation.urihttps://www.epj-conferences.org/articles/epjconf/abs/2020/15/epjconf_nd2019_06005/epjconf_nd2019_06005.htmlcs
dc.rightsCreative Commons Attribution 4.0 Internationalcs
dc.rights.accessopenAccesscs
dc.rights.sherpahttp://www.sherpa.ac.uk/romeo/issn/2100-014X/cs
dc.rights.urihttp://creativecommons.org/licenses/by/4.0/cs
dc.subjectADSen
dc.subjecttransmutationen
dc.subjectspallationen
dc.subjectproton beamen
dc.subjectJINR Dubnaen
dc.titleDistribution of neutrons and protons in elongated targetsen
dc.type.driverconferenceObjecten
dc.type.statusPeer-revieweden
dc.type.versionpublishedVersionen
sync.item.dbidVAV-166128en
sync.item.dbtypeVAVen
sync.item.insts2025.02.03 15:40:11en
sync.item.modts2025.01.17 16:40:53en
thesis.grantorVysoké učení technické v Brně. Fakulta elektrotechniky a komunikačních technologií. Ústav elektroenergetikycs
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