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Published byMaximillian Cummings Modified over 8 years ago
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Gamma Detector of the Shintake monitor 2007/12/19 Masahiro Oroku, Takashi Yamanaka H.Yoda, T.Suehara Y.Kamiya S.Komamiya(Tokyo Univ) Y.Honda, T.Tauchi, T.Kume(KEK) T.Sanuki(Tohoku Univ)
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Overview Framework of the detector Report of beam time 2007 Dec. Plans : what to do next
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Gamma detector for Shintake monitor 50mm 10mm(0.54 X 0 ) 340mm(18.4 X 0 ) 100mm CsI(Tl) crystals (from the Belle group) wrapped with teflon sheet and the Al foil
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The difference of energy distribution energy deposit in the scintillator Energy distribution of photons
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Goals of Beam Time Check the calorimeter performance Test capability to distinguish signal from background
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Layout of the test at this beam time
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Shower development from screen monitor
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Photon intensity and shower Shower development for several intensity Shower development is independent of intensity run Energy total deposit [MeV]
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Shower development with error bar layer12345 Beam Test 0.0340.0560.0840.100.73 Geant 4 0.0220.0450.0610.0720.799 Relative energy deposit
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Laser compton signals at ATF2 are considered to be similar to those from photons from laser wire We have not yet run with the laser wire on.
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conclusion Shower development of background photons is independent of the intensity Even if background at ATF2 is large, we hope that signals can be separated
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