Determination of Expected TIGERISS Observations

dc.contributor.authorRauch, B.F.
dc.contributor.authorWalsh, N.E.
dc.contributor.authorZober, W.V.
dc.contributor.authorCannady, Nicholas
dc.contributor.authorKrizmanic, John F.
dc.contributor.authorSakai, Kenichi
dc.contributor.authorTIGERISS Collaboration
dc.contributor.authoret al
dc.date.accessioned2022-08-09T21:02:02Z
dc.date.available2022-08-09T21:02:02Z
dc.date.issued2022-03-18
dc.descriptionTIGERISS Collaboration Authors: M. Alfred, M. Amoo, T. Anderson, R. G. Bose, T. J. Brandt, J. H. Buckley, N. Cannady, R. Caputo, S. Coutu, C. Kierans, J. F. Krizmanic, A. W. Labrador, J. V. Martins, J. G. Mitchell, J. W. Mitchell, S. A. I. Mognet, A. A. Moiseev, G. A. de Nolfo, S. Nutter, B. F. Rauch, K. Sakai, M. Sasaki, N. E. Walsh, L. P. Williams, and W. V. Zober
dc.description37th International Cosmic Ray Conference (ICRC 2021) July 12th – 23rd, 2021 Online – Berlin, Germanyen
dc.description.abstractWe present the method used to estimate the cosmic-ray observations expected for that the Trans-Iron Galactic Element Recorder for the International Space Station (TIGERISS), which is designed to measure the abundances of the rare Ultra-Heavy Galactic Cosmic Rays (UHCR) 30Zn and heavier. TIGERISS uses planes of crossed silicon strip detectors at the top and bottom for charge and trajectory determination and acrylic and aerogel Cherenkov detectors for velocity and charge determination. Instruments are modeled in configurations for the Japanese Experiment Module (JEM) "Kibo" Exposed Facility (∼1.66 m2 sr), as an European Space Agency Columbus Laboratory external payload (∼1.16 m2 sr), and as an ExPRESS Logistics Carrier (ELC) experiment (∼1.10 m2 sr). Differential geometry factors determined for detector orientations within the geomagnetic field over the ISS 51.6∘ inclination orbit are used to determine geomagnetic screening. Energy spectra are integrated using the higher of the energies needed to trigger the instrument or penetrate the geomagnetic field for time-weighted bins of geomagnetic latitude, instrument orientation, and incidence angle. Finally, abundances are reduced by the fraction of events calculated to fragment in the instrument.en
dc.description.urihttps://pos.sissa.it/395/088en
dc.format.extent9 pagesen
dc.genreconference papers and proceedingsen
dc.identifierdoi:10.13016/m2wea5-kuaj
dc.identifier.citation“Determination of Expected TIGERISS Observations,” B. F. Rauch, N. E. Walsh, and W. V. Zober for the TIGERISS Collaboration, Proceedings of Science: 37th International Cosmic Ray Conference , (Berlin, Germany), 088 (2021). https://doi.org/10.22323/1.395.0088en
dc.identifier.urihttps://doi.org/10.22323/1.395.0088
dc.identifier.urihttp://hdl.handle.net/11603/25331
dc.language.isoenen
dc.publisherProceedings of Scienceen
dc.relation.isAvailableAtThe University of Maryland, Baltimore County (UMBC)
dc.relation.ispartofUMBC Center for Space Sciences and Technology
dc.relation.ispartofUMBC Faculty Collection
dc.rightsPublic Domain Mark 1.0*
dc.rightsThis work was written as part of one of the author's official duties as an Employee of the United States Government and is therefore a work of the United States Government. In accordance with 17 U.S.C. 105, no copyright protection is available for such works under U.S. Law.en
dc.rights.urihttp://creativecommons.org/publicdomain/mark/1.0/*
dc.titleDetermination of Expected TIGERISS Observationsen
dc.typeTexten
dcterms.creatorhttps://orcid.org/0000-0003-2916-6955en

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