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We thus can identify charge redistribution as the primary SD mechanism, with a smaller but important contribution (17% of original SD) from carbon oxidation.
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Results obtained by frequency response analysis and by polarization curves, were used to identify charge-transfer resistance, double layer capacity and properties of passivation films.
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.
We describe the design, construction and performance of a Ring Imaging Cherenkov Detector (RICH) constructed to identify charged particles in the CLEO experiment.
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].
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).
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