PPT-The silicon strip vertex detector of the Belle II experiment

Author : nersonvisa | Published Date : 2020-08-03

Yoshiyuki Onuki On behalf of BelleII SVD collaboration University of Tokyo Kavli IPMU 1 201393 9th International Hiroshima Symposium on the Development and Application

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The silicon strip vertex detector of the Belle II experiment: Transcript


Yoshiyuki Onuki On behalf of BelleII SVD collaboration University of Tokyo Kavli IPMU 1 201393 9th International Hiroshima Symposium on the Development and Application of Semiconductor Tracking Detectors Hiroshima Japan. Au+Au. collisions at √. s. NN. = 200 . GeV. in STAR experiment at RHIC. Jaiby Joseph Ajish. 11/9/2011. Outline. Introduction. Why collide nuclei at high energies?. RHIC and STAR. Physics at RHIC. Preshower. for the CMS: BARC Participation . Anita . Topkar. BARC. CMS Preshower Detector. End caps of . CMS detector has ~4300 . silicon . strip detectors covering . area . of~17 . m. 2 . . BARC . Detector. Markus Friedl (HEPHY Vienna) . for. . the. Belle II SVD Group. VCI, 13 . February. 2013. 13 February 2013. M.Friedl (Belle II SVD Group): The Belle II SVD. 2. Introduction. Front-End. Electronics. NN. = 200 GeV in STAR experiment at RHIC. Jaiby Joseph . Ajish. 11/2/2011. Outline. Quick summary of my contributions. Introduction. Why . collide nuclei at high energies?. RHIC, STAR. Physics at RHIC. Au+Au. collisions at √. s. NN. = 200 . GeV. in STAR experiment at RHIC. Jaiby Joseph Ajish. 11/9/2011. Outline. Introduction. Why collide nuclei at high energies?. RHIC and STAR. Physics at RHIC. NN. = 200 GeV in STAR experiment at RHIC. Jaiby Joseph . Ajish. 11/2/2011. Outline. Quick summary of my contributions. Introduction. Why . collide nuclei at high energies?. RHIC, STAR. Physics at RHIC. Hrvoje Štefančić. . Theoretical Physics Division . Ruđer Bošković Institute . (based on joint work with . Hrvoje Abraham . and . Predrag Lazić. ). Electric field strength in a segment of a Si microstrip detector. SuperKEKB. and Belle II Upgrades. Tom Browder. University of Hawaii . B Mesons: . “. Laboratory Rats of the Weak Interaction. ”. Exotic bound state of matter and antimatter. (hydrogen-like). b quark mass . AGH University of Science and Technology. . Faculty of Physics and Applied Computer Science, . Kraków. , Poland. Jagiellonian. . Symposium. 2015 7-12/06/2015. Au Au. collisions at √. s. NN. = 200 . GeV. in STAR experiment at RHIC. Jaiby Joseph Ajish. 11/9/2011. Outline. Introduction. Why collide nuclei at high energies?. RHIC and STAR. Physics at RHIC. guardring. Dimension Details. 6750um (active edge boundaries). 6500um active width (130strips x 50um). Entrance window for x-rays. 2415um. Pad . layout for . strip . detector w/surrounding Guard Ring . Jan . Kaplon. CERN, . Geneva . Outline. S. ilicon strip detectors for the High Luminosity LHC upgrade . Requirements and constraints. Basic architectures of the input stages. Examples of the channel architecture for ATLAS and CMS . stack. Introduction . RPC detector and gas composition . Signal and noise in RPC. Muon trajectory. Zenith and azimuthal distribution of muon. Conclusion. Gobinda Majumder, TIFR, Mumbai. INO collaboration. 01.02.2016. Dorothea . Pfeiffer. NMX detectors. 2. Gd-GEM backwards setup. 13.11.2014. Dorothea Pfeiffer. 3. neutron. c. onversion electron. Start of track. α . particle and electron . t. racks. Whereas .

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