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Michael,
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<div>One more thing should be taken into account. In CLAS12 Liquid Hydrogen target will be 5cm long compared</div>
<div>to 40cm used for example in g11 run.</div>
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<div>This makes expected count rate probably very similar to CLAS6, one should be very careful to not overstate.</div>
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<div>Best regards,</div>
<div>Moskov.</div>
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<div>On Sep 8, 2015, at 12:09 PM, Michael C. Kunkel <<a href="mailto:mkunkel@jlab.org">mkunkel@jlab.org</a>> wrote:</div>
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<blockquote type="cite">Greetings,<br>
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I see that I was low by one order of magnitude, which means my total events seen should be higher than when I presented.<br>
Either way, the number of eta' dalitz decays in CLAS12 exceeds previous CLAS numbers.<br>
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This is mostly due to the increase of efficiency of CLAS and also the amount of particles traversing through e+e- detection due to lorentz boost.<br>
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BR<br>
MK<br>
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Michael C. Kunkel, PhD<br>
Forschungszentrum Jülich<br>
Nuclear Physics Institute and Juelich Center for Hadron Physics<br>
Experimental Hadron Structure (IKP-1)<br>
<a href="http://www.fz-juelich.de/ikp">www.fz-juelich.de/ikp</a><br>
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On 9/8/15 5:33 PM, Amaryan, Moskov wrote:<br>
<blockquote type="cite">N_gamma = 60*10^{-9}*10^{-3}/(1.6*10^{-19} ~ 4*10^8<br>
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Prof. Moskov Amaryan<br>
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Department of Physics</div>
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