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. 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. 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?. CLAS and CLAS11. Paul Stoler-RPI. Measure . electroproduction. of mesons above the. resonance region (W > 2 . GeV. ) over a large range of. of . Q. 2. and . t. in the valence quark region of . x. T. Sato Osaka U./KEK . Motivation. Analysis of meson production reaction and dynamical coupled channel model. extracting resonance parameters. Resonance mass and width. Role of reaction dynamics on resonance properties. GeV. for IDS120h (Update). X. Ding, UCLA. AAG Meeting, Jan. 26, 2012. 1. Configuration of IDS120h. 2. Field Map of IDS120h. (. Bz. at . r. = 0). 3. Meson Production Study. The . mercury jet target geometry. The proton beam and mercury jet cross at . 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. 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.. . Lee . . . 1. Few words on a recent sum rule result. 2. A simple constituent quark model for D meson . 3. Consequences . 4. Summary. D meson in nuclear medium: a . consituent. Aps. :. 1) GSI cross . secs. , & 2) nuclear forces. Ted Barnes. Physics Div. ORNL and. Dept. of Physics, . U.Tenn. .. . (. and . p.t. . DOE ONP. ). . INT Nov 2009 . 1. For PANDA: Associated . 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.