PPT-Charmed Meson measurements using a Silicon Tracker in

AuAu collisions at s NN 200 GeV in STAR experiment at RHIC Jaiby Joseph Ajish 1192011 Outline Introduction Why collide nuclei at high energies RHIC and STAR Physics at RHIC. desyde On behalf of the H1 and ZEUS collaborations Recent results from the H1 and ZEUS collaborations on charmed meson production in deep in elastic scattering at HERA are presented Single dif ferential cross sections of and meson production are meas April 20, 2015. ASRC Seminar. 1. Atsushi . Hosaka. , RCNP, Osaka. ASRC Seminar. Contents. 1. Introduction. 2. Structure: . How . ρλ. modes . appear in . the spectrum. 3. . C. harmed baryon productions and decays. 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. JLab. Curtis A. Meyer. Carnegie Mellon University. August 2009. Charmed Exotics. 2. Outline. What are light-quark exotic mesons?. How should we look for these mesons?. What is the Experimental Evidence?. in . ep. . missing. . spectra. G. M. Urciuoli. M. eson . photoproduction. provide a good tool to study nucleon resonances. . For example, a . large number of resonances predicted by the constituent quark model . Dan Watts. University of Edinburgh. Outline. Many proton knockout. Nuclear tagging using nuclear gamma decay photons. Recoil nucleon spin . polarimetry. – first crude look at possibilities. Many nucleon knockout from nuclei. 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. rate. s . of . Strange. and Charmed baryons . at Belle. 1. string. @. . s = 10.52 GeV. Nuclear physics consortium . Production rate. . of hadrons. . 2. Slope of meson (qq. bar. ) . is different from baryons (qqq). . Silicon Pixel Tracker – Chris Damerell. 1. The Silicon Pixel Tracker – beginning of a revolution?. Chris Damerell (RAL). SPT concept was first presented by Konstantin Stefanov in March 2008. He was made redundant by STFC shortly afterwards, but internationally, interest in the SPT has grown steadily, not only for the linear collider.. 孙宝玺. . 北京工业大学. . . 合作者. : . 吕晓夫 四川大学. . . FHNP’15. 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. Silicon wafer. www.guardian.co.uk. http://. mrsec.wisc.edu. en.wikipedia.org. Wafers are cut from . boules. , . which are large . logs . of uniform . silicon.. Looking at this picture, . where. do you think silicon . Phil Allport,. . Matt . B. aca, James Broughton, Andy Chisholm, Laura Gonella, Kostas Nikolopoulos, Simon Pyatt, Juergen Thomas, John Wilson. . 30/09/15. 1. Introduction. ATLAS UK Tracker Upgrade. with. SIDDHARTA . by Johann Zmeskal. SMI, Vienna. MESON 2012. 12th International Workshop on Meson Production, Properties and Interaction. KRAKÓW, POLAND. 31 May - 5 June 2012. MESON 2012. LNF- INFN, .