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Table 3 The slope b resulting from a fit to the differential cross-section /dt to an exponential form for the reaction γ*pρ0p, for different Q2 intervals. The first column gives the Q2 bin, while the second column gives the Q2 value at which the differential cross sections are quoted. The first uncertainty is statistical, the second systematic.

From: Exclusive ρ0 production in deep inelastic scattering at HERA

Q2 bin (GeV2) Q2 (GeV2) b (GeV-2)
2–4 2.7 6.6 ± 0.1 0.2 + 0.2 MathType@MTEF@5@5@+=feaafiart1ev1aaatCvAUfKttLearuWrP9MDH5MBPbIqV92AaeXatLxBI9gBaebbnrfifHhDYfgasaacH8bkY=wiFfYlOipiY=Hhbbf9v8qqaqFr0xc9vqpe0di9q8qqpG0dHiVcFbIOFHK8Feei0lXdar=Jb9qqFfeaYRXxe9vr0=vr0=LqpWqaaeaabiGaaiaacaqabeaabeqacmaaaOqaaiabiAda2iabc6caUiabiAda2iabgglaXkabicdaWiabc6caUiabigdaXmaaDaaaleaacqGHsislcqaIWaamcqGGUaGlcqaIYaGmaeaacqGHRaWkcqaIWaamcqGGUaGlcqaIYaGmaaaaaa@3A01@
4–6.5 5.0 6.3 ± 0.2 0.2 + 0.2 MathType@MTEF@5@5@+=feaafiart1ev1aaatCvAUfKttLearuWrP9MDH5MBPbIqV92AaeXatLxBI9gBaebbnrfifHhDYfgasaacH8bkY=wiFfYlOipiY=Hhbbf9v8qqaqFr0xc9vqpe0di9q8qqpG0dHiVcFbIOFHK8Feei0lXdar=Jb9qqFfeaYRXxe9vr0=vr0=LqpWqaaeaabiGaaiaacaqabeaabeqacmaaaOqaaiabiAda2iabc6caUiabiodaZiabgglaXkabicdaWiabc6caUiabikdaYmaaDaaaleaacqGHsislcqaIWaamcqGGUaGlcqaIYaGmaeaacqGHRaWkcqaIWaamcqGGUaGlcqaIYaGmaaaaaa@39FD@
6.5–10 7.8 5.9 ± 0.2 0.2 + 0.2 MathType@MTEF@5@5@+=feaafiart1ev1aaatCvAUfKttLearuWrP9MDH5MBPbIqV92AaeXatLxBI9gBaebbnrfifHhDYfgasaacH8bkY=wiFfYlOipiY=Hhbbf9v8qqaqFr0xc9vqpe0di9q8qqpG0dHiVcFbIOFHK8Feei0lXdar=Jb9qqFfeaYRXxe9vr0=vr0=LqpWqaaeaabiGaaiaacaqabeaabeqacmaaaOqaaiabiwda1iabc6caUiabiMda5iabgglaXkabicdaWiabc6caUiabikdaYmaaDaaaleaacqGHsislcqaIWaamcqGGUaGlcqaIYaGmaeaacqGHRaWkcqaIWaamcqGGUaGlcqaIYaGmaaaaaa@3A07@
10–15 11.9 5.5 ± 0.2 0.2 + 0.2 MathType@MTEF@5@5@+=feaafiart1ev1aaatCvAUfKttLearuWrP9MDH5MBPbIqV92AaeXatLxBI9gBaebbnrfifHhDYfgasaacH8bkY=wiFfYlOipiY=Hhbbf9v8qqaqFr0xc9vqpe0di9q8qqpG0dHiVcFbIOFHK8Feei0lXdar=Jb9qqFfeaYRXxe9vr0=vr0=LqpWqaaeaabiGaaiaacaqabeaabeqacmaaaOqaaiabiwda1iabc6caUiabiwda1iabgglaXkabicdaWiabc6caUiabikdaYmaaDaaaleaacqGHsislcqaIWaamcqGGUaGlcqaIYaGmaeaacqGHRaWkcqaIWaamcqGGUaGlcqaIYaGmaaaaaa@39FF@
15–30 19.7 5.5 ± 0.3 0.3 + 0.2 MathType@MTEF@5@5@+=feaafiart1ev1aaatCvAUfKttLearuWrP9MDH5MBPbIqV92AaeXatLxBI9gBaebbnrfifHhDYfgasaacH8bkY=wiFfYlOipiY=Hhbbf9v8qqaqFr0xc9vqpe0di9q8qqpG0dHiVcFbIOFHK8Feei0lXdar=Jb9qqFfeaYRXxe9vr0=vr0=LqpWqaaeaabiGaaiaacaqabeaabeqacmaaaOqaaiabiwda1iabc6caUiabiwda1iabgglaXkabicdaWiabc6caUiabiodaZmaaDaaaleaacqGHsislcqaIWaamcqGGUaGlcqaIZaWmaeaacqGHRaWkcqaIWaamcqGGUaGlcqaIYaGmaaaaaa@3A03@
30–80 41.0 4.9 ± 0.6 0.5 + 0.8 MathType@MTEF@5@5@+=feaafiart1ev1aaatCvAUfKttLearuWrP9MDH5MBPbIqV92AaeXatLxBI9gBaebbnrfifHhDYfgasaacH8bkY=wiFfYlOipiY=Hhbbf9v8qqaqFr0xc9vqpe0di9q8qqpG0dHiVcFbIOFHK8Feei0lXdar=Jb9qqFfeaYRXxe9vr0=vr0=LqpWqaaeaabiGaaiaacaqabeaabeqacmaaaOqaaiabisda0iabc6caUiabiMda5iabgglaXkabicdaWiabc6caUiabiAda2maaDaaaleaacqGHsislcqaIWaamcqGGUaGlcqaI1aqnaeaacqGHRaWkcqaIWaamcqGGUaGlcqaI4aaoaaaaaa@3A1F@