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Measurement of Photoproduction of (1020) Mesons on Protons by Linearly Polarized Photons EMI2001, December 5th, 2001 T.Mibe for the LEPS collaboration Research Center for Nuclear Physics, Osaka University, Japan
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Outline photoproduction near production threshold Experiment at SPring-8/LEPS facility Summary
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Vector Meson Photoproduction Vector Meson Dominance Meson Exchange Pomeron Exchange N N q _q_q _ qq = Dominant at low energies Small energy dependence
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Cross section of Vector Meson Photoproduction p p p p M.A. Pichowsky and T.-S. H. Lee PRD 56, 1644 (1997) Data from: LAMP2('83), DESY('76), SLAC('73), CERN('82), FNAL('79,'82), ZEUS('95,'96) Prediction from Pomeron exchange Prediction from meson exchange
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photoproduction near production threshold Titov, Lee, Toki Phys.Rev C59(1999) 2993 P2 : 2 nd pomeron ~ 0 + glueball (Nakano, Toki (1998))
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Photoproducion by linearly polarized photon Decay Plane // if natural parity exchange (-1) J (Pomeron, Scaler mesons) Polarization vector of K+K+ K-K- K+K+ K-K- Decay Plane if unnatural parity exchange -(-1) J (Pseudoscaler mesons) In rest frame (Helicity frame) Decay Angular distribution of Decomposition of natural parity exchange unnatural parity exchange
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Angles In rest frame (Helicity frame) In center-of-mass frame
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At high energies... p p E = 9.3 GeV Linear Pol. Ballam et.al. PLD 7(1973) 3150 tends to decay into direction of the photon polarizaion. Natural parity exchange dominate s-channel helicity is conserved. What is the situation in p p near threshold ??? LEPS,Spring-8 CLAS,J.lab. - pol (degree)
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LEPS collaboration Academia Sinica, Taiwan W.C.Chang, D.S.Oshuev, C.W.Wang, S.C.Wang Chiba University, Japan H.Kawai, T.Ooba, Y.Shiino IHEP, Russia P.Shagin JAERI, Japan Y.Asano, N.Muramatsu, R.G.T.Zegers JASRI, Japan S.Date, N.Kumagai, Y.Ohashi, H.Ookuma Konan University, Japan H.Akimune Kyoto University, Japan K.Imai, T.Ishikawa, M.Miyabe, M.Niiyama, M.Yosoi Nagoya University, Japan S.Fukui, T.Iwata, Y.Miyachi, A.Wakai Ohio University, U.S. K.Hicks Osaka University, Japan M.Nomachi, A.Sakaguchi, Y.Sugaya, M.Sumihama Pusan National University, S.Korea J.K.Ahn RCNP, Osaka University, Japan H.Fujimura, M.Fujiwara, T.Hotta, H.Kohri, T.Matsumura, N.Matsuoka, T.Mibe, M.Morita, T.Nakano, T.Yorita Saskatchewan University, Canada C.Rangacharyulu Tohoku University, Japan H.Shimizu Wakayama Med. University, Japan S.Makino
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Linearly polarized Photon Tagging Region : 1.5 GeV< E < 2.4 GeV Intensity (Typ.) : 5 * 10 5 cps Linear Polarization : 95 % at 2.4 GeV E (Tagger) (GeV) E (GeV) Counts Degree of Polarization QED calculation
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LEPS detectors 1m1m TOF wall MWDC 2 MWDC 3 MWDC 1 Dipole Magnet (0.7 T) Liquid Hydrogen Target (50mm thick) Start counter Silicon Vertex Detector Aerogel Cerenkov (n=1.03)
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LH 2 target Runs Physics Run : Dec.2000 - June.2001 Number of mesons More than ~5200 ’ s = (1800 +400 +400) *2 Plots in this talk : K + K - mode only, ~30 % of total data K + K - detected K + p detected K - p detected Polarization(Vert./Hori.)
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K + K - events invariant mass (GeV) missing mass (GeV) Number of event /2MeV Number of event /5MeV p(938) Preliminary Reconstructed mass distributions from K + K - tracks
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p p 554 events (Vert + Hori) 1.004< M <1.034 GeV 0.88<Missing mass<1.00 GeV -0.2< t <0.0 GeV 2 w/o Acceptance Correction Decay angular distribution of K + in Helicity frame Preliminary K - pol (degree) cos h Number of event
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Summary Photoproduction of mesons near threshold opens a window to access new mechanisms in addition to the pomeron exchange. photoproduction is measured with linearly polarized photon beam from E = 1.6GeV(threshold) to 2.4GeV at SPring-8. The azimuthal angle distribution of K+ from decay shows non flat distribution with respect to the photon polarization. The s-channel helicity conservation is favoured.
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