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This approach relies on identifying charge states based on the observed C isotope spacing [90], or identifying oligomer size based on unique, odd numbered charge states [88,89].
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The background rates differ between the BI and the FI chips, in part because of differences in the efficiency for identifying charged particle interactions.
Photoluminescence (PL) spectroscopy and time-correlated single photon counting (TCSPC) have been commonly used to understand charge collection efficiencies and identify charge transfer mechanisms.
We thus can identify charge redistribution as the primary SD mechanism, with a smaller but important contribution (17% of original SD) from carbon oxidation.
The linear dependence of Rxy(B) with positive slope identifies charge carriers as holes, with a Hall carrier density n H = B/ eRxy) = 3 × 10cm−2 (see Figure 1c).
The proximity-focusing A-RICH system is especially designed to identify charged kaons and pions.
Each calorimeter is equipped with a plastic scintillator hodoscope to identify charged particles.
It has been designed to identify charged pions and kaons in the range 1⩽p⩽3Gev/c and protons in the range 2⩽p⩽5Gev/c.
It has been designed to identify charged pions and kaons in the range 1< pt <3GeV/c and protons in the range 2< pt <5GeV/c.
The DIRC-like TOF detector is a ring imaging Cherenkov counter, designed for the SuperB experiment, which uses time-of-flight to identify charged particles.
The ALICE HMPID (High Momentum Particle IDentification) detector has been designed to identify charged pions and kaons in the range 1÷3GeV/c and protons in the range 1.5÷5GeV/c.
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