PDF-Properties of the positron

K W K positrons are positively charged high sensitivity to detect and identify atomic scale defects Positron Science Particle Physics The positron and its antiparticle the electron are elem. Tzu-Cheng, Chuang. . (. 莊子承. ). Exchange student from. National Tsing-Hua University (Taiwan). (. 國立清華大學. , . 台灣. ). Where?. Russia. China. Japan. Taiwan. Zoom in. China. Hong Kong. Chemistry. ________________ involve changes with electrons. . ________________ involve changes in atomic nuclei. . Spontaneously-changing nuclei emit ________ and. are said to be _________. . Chemical reactions. . LCWS . 2014, Belgrade, October 6. th. -10. th. , . 2014. Steffen Döbert, BE-RF. No changes to the electron injector. Some work started on optimizing the. positron source with a student started recently . Wei Gai for the ILC e- and e+ collaboration . PAC review, 2012. KEK, Japan. ILC site layout and location of e- and e+ sources. Page . 3. The Baseline ILC Electron Source . Electron source provides polarized electron beam and consists of all systems from source laser to 5 GeV injection to damping rings. ( 325 MHz SHB). R.CHEHAB (IPNL). On behalf of . I.Chaikovska. (LAL), . H.Guler. (LAL), . P.Bambade. (LAL), . O.Bianco. (LAL), . F.Plassard. (LAL), . X.Artru. (IPNL), . M.Chevallier. (IPNL), . J.Gao. (IHEP), . Shannon . Fogwell. . Hoogerheide. Lepton Moments 2014. July 21, 2014. Acknowledgements. 2. Prof. Gerald . Gabrielse. Elise . Novitski. (PhD in progress…). Joshua Dorr (2013). Shannon . Fogwell. . for Measurements of. . G. eneralized . P. arton . D. istributions. e. +. @ . JLab. Generalized . parton. distributions. Polarized positron production. Polarization transfer physics. . PEPPo. at room temperature. J. . Kansy. 1. . and M. Ziąbka. 2. .  . 1. . Institute of Material Science, Silesian University, . Bankowa. 12, 40-008 Katowice, . Poland. 2. . Faculty of Materials Science and Ceramic, University of Science and Technology, A. . 実験に. おける. 陽電子. 再構成アルゴリズムの. 開発. Development . of positron reconstruction algorithm in MEG II experiment. 西村美紀（東大）. 他　. MEGII. コラボレーション. Studen. , . Karol . Brzezinski. , . Enrico. . Chesi. , Vladimir . Cindro. , . Neal. H. . Clinthorne. , Milan . Grkovski. , Borut . Grošičar. , Klaus . Honscheid. ,. . S. S. . Huh. , Harris . Kazuro Furukawa. for Injector Linac. 1. 概要. Alignment. 電子銃. RF . 電子銃. 熱電子銃. 陽電子発生装置. Schedule. 2. Linac Upgrade Overview. 3. 40-times higher Luminosity. Twice larger storage beam . GeV electron beam in less than one meter of plasmaGeV energy gain of a positron beam in one metre of plasma and the laser-driven acceleration of electrons up to 8 GeV in only 20cm of plasma anks to it IAEA 2 FIG 1 The configuration of the positron source of POSH Four disks are shown at the right side In the disks made from tungsten foils the pair formation from hard gammas emerging from the reacto 16 – 20 March 2015. Cosmic Rays: the current position -. from AMS to the Auger Observatory. 1. Alan Watson. University of Leeds. a.a.watson@leeds.ac.uk. Lecture 1:. Overview of the cosmic ray scene.