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Introduction to the E391a.

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Presentation on theme: "Introduction to the E391a."— Presentation transcript:

1 Introduction to the E391a

2 E391a Collaboration High Energy Accelerator Research Organization, KEK, Japan Joint  Institute for Nuclear Research (Dubna), Russia Department of Physics, Kyoto University, Japan National Defense Academy of Japan, Japan Department of Physics, National Taiwan University, Taiwan Department of Physics, Osaka University, Japan Department of Physics, Pusan National University, Korea Research Center for Nuclear Physics, Osaka University, Japan Faculty of Science and Engineering, Saga University, Japan Department of Physics, University of Chicago, USA Department of Physics, Yamagata University, Japan

3 KLgp0nn physics Flavor Changing Neutral Current
Direct CP violation (Ds =1)    Im(Vtd) measurement Very small theoretical ambiguity    Only top loop in SM     clean and pure Last frontier in K-decay    challenging

4 Experimental situation - Current and future -

5 Mile stones Dec.1996: conditionally approved
Mar.1999: constructed the beam line July 2001: approved Oct. 2002: engineering run Nov.2003: middle section (last vacuum           chamber) arrived 18 Feb. 2004: Started data taking

6 Detection Method Pencil Beam Pencil beam
Detector with complete veto system 4p coverage with thick calorimeter Wide acceptance Double decay chamber Operation in high vacuum High PT selection Step by step approach KEK-PS E391a JPARC Detector system

7 Detector system

8 Detector system (Cont.)

9 Detector Integration Jan 22, 2004

10 Calibration using cosmic rays

11 Clearly reconstructed KL decay modes
KL  p0p0p0 KL  p0p0 6-g invariant mass (GeV/c2) 4-g invariant mass (GeV/c2)

12 JPARC

13 A-line plan at JPARC


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