PPT-R&D ON POSITRON AND ELECTRON BEAMS FOR FUTURE COLLIDE

RCHEHAB IPNL On behalf of IChaikovska LAL HGuler LAL PBambade LAL OBianco LAL FPlassard LAL XArtru IPNL MChevallier IPNL JGao IHEP . Ady Arie. Dept. of Physical Electronics. , . Tel-Aviv University, Tel-Aviv, . Israel. Heraklion. , Crete, September 20. th. 2013. 2. Outline. The quantum-mechanical Airy wave-function and its properties. 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. Roberta Sparvoli. Rome . “. Tor Vergata. ”. . University. and . INFN, ITALY. PCC 2011 - CERN. SIGNALS . from. RELIC . WIMPs. Direct . searches. :. . elastic. . scattering. of a WIMP off detector . collapses. In . collaboration. . with. . Wen-Biao. Han, & Remo . Ruffini. . ICRANet. & . Physics. . Department. , . University. . of. . Rome. She-Sheng. . Xue. MG13, Stockholm, July 5. Chemistry. ________________ involve changes with electrons. . ________________ involve changes in atomic nuclei. . Spontaneously-changing nuclei emit ________ and. are said to be _________. . Chemical reactions. 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). for Measurements of. . G. eneralized . P. arton . D. istributions. e. +. @ . JLab. Generalized . parton. distributions. Polarized positron production. Polarization transfer physics. . PEPPo. Momenta. , Geometric Phases,. and Spin-Orbit Interactions . of Light and Electron Waves. Konstantin Y. . Bliokh. Advanced . Science Institute, RIKEN, Wako-. shi. , Saitama, Japan . . In collaboration with:. Physical Principles and Dosimetry. Kent A. Gifford, Ph.D.. Department of Radiation Physics. UT M.D. Anderson Cancer Center. kagifford@mdanderson.org. Medical Physics III: Spring . 2015. Physical aspects. Ady Arie. Dept. of Physical Electronics. , . Tel-Aviv University, Tel-Aviv, . Israel. Heraklion. , Crete, September 20. th. 2013. 2. Outline. The quantum-mechanical Airy wave-function and its properties. 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 . Intra-beam . Scattering. Mauro Pivi, MedAustron - work made while at SLAC -. i. n . collaboration. with: T. . Demma. (Frascati & LAL), the ILC / CLIC and . 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 beta decay. . They are designated by beta (β). There are two forms of beta decay, . β. −.  and . β. +. , which respectively give rise to the electron and the positron.. . The generalized atomic equation for beta decay is as follows.