13–17 Jun 2011
Künstlerhaus
Europe/Berlin timezone
Proceedings are now available online at <a href="http://www.slac.stanford.edu/econf/C110613/">eConf</a>

Session

Future Experiments

16 Jun 2011, 14:30
Künstlerhaus

Künstlerhaus

Lenbachplatz 8, D-80333 München

Conveners

Future Experiments

  • Bernhard Ketzer (TUM)

Presentation materials

There are no materials yet.

  1. Prof. Peter Krizan (University of Ljubljana)
    16/06/2011, 14:30
    Future Experiments
    talk
    The talk discusses future experiments in hadron spectroscopy. It presents the physics motivation and the tools, accelerators and detectors, and reviews the status of the relevant projects, Belle-II/SuperKEKB at KEK, SuperB in Italy, PANDA at FAIR, and CLAS12 and GlueX at JLAB.
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  2. Dr J.H. Lee (Brookhaven National Laboratory)
    16/06/2011, 14:55
    Future Experiments
    talk
    Nuclei and nucleons probed in DIS and diffractive processes in the high-energy (low-x) regime open a new precision window into fundamental questions in QCD. The proposed Electron-Ion Collider at BNL (eRHIC) is a new high-energy and high-luminosity polarized electron-ion/polarized proton machine. The proposed design provides unprecedented access to study deeply the nature of QCD matter...
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  3. Dr Masayuki Niiyama (Kyoto Univ.)
    16/06/2011, 15:15
    Future Experiments
    talk
    The construction of a new backward Compton gamma ray beam line at SPring-8 in Japan, LEPS2, has been started from the year 2010. The new beam line will provide a highly polarized photon beam up to 3 GeV with 10 times higher intensity than that of LEPS1 facility. We will construct a 4$\pi$ detector which can detect both of charged particles and photons. The photon beam will be...
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  4. Igor Senderovich (University of Connecticut)
    16/06/2011, 15:35
    Future Experiments
    talk
    The GlueX experiment will employ a linearly polarized 9GeV tagged photon beam incident on a liquid hydrogen target to search for exotic states in the light meson spectrum. Optimized for this purpose, the detector has a highly uniform acceptance over nearly 4\pi solid angle, with high efficiency for both neutral and charged final state particles. An overview of the physics motivation and...
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