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We present a measurement of the ratio of events with correlated t and tbar spins to the total number of ttbar events.
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The pseudorapidity η \eta is defined relative to the center of the detector as η = − ln [ tan ( θ / 2 ) ] \eta=-\ln[\tan(\theta/2)] where θ \theta is the polar angle with respect to the proton beam direction
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We do not use MEs for the smaller g g → t t ¯ gg\rightarrow t\bar{t} contribution in the calculation of P sgn P_{\rm sgn} , but account for it in the measurement by using NLO t t ¯ t\bar{t}
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