Zobrazeno 1 - 4
of 4
pro vyhledávání: '"Beomki Yeo"'
Autor:
Xiaocong Ai, Corentin Allaire, Noemi Calace, Angéla Czirkos, Markus Elsing, Irina Ene, Ralf Farkas, Louis-Guillaume Gagnon, Rocky Garg, Paul Gessinger, Hadrien Grasland, Heather M. Gray, Christian Gumpert, Julia Hrdinka, Benjamin Huth, Moritz Kiehn, Fabian Klimpel, Bernadette Kolbinger, Attila Krasznahorkay, Robert Langenberg, Charles Leggett, Georgiana Mania, Edward Moyse, Joana Niermann, Joseph D. Osborn, David Rousseau, Andreas Salzburger, Bastian Schlag, Lauren Tompkins, Tomohiro Yamazaki, Beomki Yeo, Jin Zhang
The reconstruction of the trajectories of charged particles, or track reconstruction, is a key computational challenge for particle and nuclear physics experiments. While the tuning of track reconstruction algorithms can depend strongly on details of
Externí odkaz:
https://explore.openaire.eu/search/publication?articleId=doi_dedup___::ff10c41873579cf2c503bc0c78ab42ce
http://cds.cern.ch/record/2775922
http://cds.cern.ch/record/2775922
Publikováno v:
Proceedings of The 39th International Conference on High Energy Physics — PoS(ICHEP2018).
Track finding with GPU-implemented fourth order Runge-Kutta (RK) method is investigated to track electrons from muon decay in the COMET drift chamber. In the COMET drift chamber, about 30-40 \% of signal events are composed of multiple turns where th
This paper discusses a parallelized event reconstruction of the COMET Phase-I experiment. The experiment aims to discover charged lepton flavor violation by observing 104.97 MeV electrons from neutrinoless muon-to-electron conversion in muonic atoms.
Externí odkaz:
https://explore.openaire.eu/search/publication?articleId=doi_dedup___::af0b4168adceeebeaef67cb684a1ebca
Future experimental improvement for the search of lepton-number-violating processes in the eμ sector
Publikováno v:
Physical Review D. 96
The conservation of lepton flavor and total lepton number are no longer guaranteed in the Standard Model after the discovery of neutrino oscillations. The ${\ensuremath{\mu}}^{\ensuremath{-}}+N(A,Z)\ensuremath{\rightarrow}{e}^{+}+N(A,Z\ensuremath{-}2