PCarbon normalization

		B1U	B2D	Y1D	Y2U
		$k={\frac {P_{\text{H-jet}}}{P_{\text{p-Carbon}}}}\pm \Delta k$

Run 13	24 GeV	1.06 ± 0.02	1.11 ± 0.03	1.09 ± 0.02	1.08 ± 0.03
	255 GeV	0.9824 ± 0.0104	0.9671 ± 0.009	0.9552 ± 0.0094	0.9503 ± 0.0099

Run 12	24 GeV			1.02 ± 0.07	0.99 ± 0.02
	100 GeV	1.03 ± 0.01	1.14 ± 0.02 ^[1]	1.03 ± 0.02	0.99 ± 0.02
	255 GeV	0.98 ± 0.01	1.14 ± 0.03 ^[1]	1.08 ± 0.02	1.02 ± 0.02

Run 11	24 GeV
Run 11	250 GeV	0.95 ± 0.01	1.09 ± 0.02 ^[2]	0.94 ± 0.02	0.95 ± 0.01

Run 9	31 GeV
	100 GeV	1.00 ± 0.02	0.98 ± 0.01	1.01 ± 0.01	1.02 ± 0.01
	250 GeV	0.88 ± 0.03	0.86 ± 0.03	0.91 ± 0.03	0.88 ± 0.03

↑ ^1.0 ^1.1 In Run 12 the B2D polarimeter had two detectors with strips oriented perpendicular to the beam
↑ This scale includes measurements with thick target(s) which could shift the energy range for A_N

Last modified by Elke on 13-03-2015

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