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Table 11 The values of the effective Pomeron trajectory intercept α(0) and slope α MathType@MTEF@5@5@+=feaafiart1ev1aaatCvAUfKttLearuWrP9MDH5MBPbIqV92AaeXatLxBI9gBaebbnrfifHhDYfgasaacH8bkY=wiFfYlOipiY=Hhbbf9v8qqaqFr0xc9vqpe0di9q8qqpG0dHiVcFbIOFHK8Feei0lXdar=Jb9qqFfeaYRXxe9vr0=vr0=LqpWqaaeaabiGaaiaacaqabeaabeqacmaaaOqaaGGaciqb=f7aHzaafaWaaSbaaSqaamrr1ngBPrwtHrhAYaqeguuDJXwAKbstHrhAGq1DVbaceaGae4xgHafabeaaaaa@3783@ , for two Q2 values. The first uncertainty is statistical, the second systematic.

From: Exclusive ρ0 production in deep inelastic scattering at HERA

Q2 bin (GeV2) Q2(GeV2) α(0) α MathType@MTEF@5@5@+=feaafiart1ev1aaatCvAUfKttLearuWrP9MDH5MBPbIqV92AaeXatLxBI9gBaebbnrfifHhDYfgasaacH8bkY=wiFfYlOipiY=Hhbbf9v8qqaqFr0xc9vqpe0di9q8qqpG0dHiVcFbIOFHK8Feei0lXdar=Jb9qqFfeaYRXxe9vr0=vr0=LqpWqaaeaabiGaaiaacaqabeaabeqacmaaaOqaaGGaciqb=f7aHzaafaWaaSbaaSqaamrr1ngBPrwtHrhAYaqeguuDJXwAKbstHrhAGq1DVbaceaGae4xgHafabeaaaaa@3783@ (GeV-2)
2–5 3 1.113 ± 0.010 0.012 + 0.009 MathType@MTEF@5@5@+=feaafiart1ev1aaatCvAUfKttLearuWrP9MDH5MBPbIqV92AaeXatLxBI9gBaebbnrfifHhDYfgasaacH8bkY=wiFfYlOipiY=Hhbbf9v8qqaqFr0xc9vqpe0di9q8qqpG0dHiVcFbIOFHK8Feei0lXdar=Jb9qqFfeaYRXxe9vr0=vr0=LqpWqaaeaabiGaaiaacaqabeaabeqacmaaaOqaaiabigdaXiabc6caUiabigdaXiabigdaXiabiodaZiabgglaXkabicdaWiabc6caUiabicdaWiabigdaXiabicdaWmaaDaaaleaacqGHsislcqaIWaamcqGGUaGlcqaIWaamcqaIXaqmcqaIYaGmaeaacqGHRaWkcqaIWaamcqGGUaGlcqaIWaamcqaIWaamcqaI5aqoaaaaaa@4175@ 0.185 ± 0.042 0.057 + 0.022 MathType@MTEF@5@5@+=feaafiart1ev1aaatCvAUfKttLearuWrP9MDH5MBPbIqV92AaeXatLxBI9gBaebbnrfifHhDYfgasaacH8bkY=wiFfYlOipiY=Hhbbf9v8qqaqFr0xc9vqpe0di9q8qqpG0dHiVcFbIOFHK8Feei0lXdar=Jb9qqFfeaYRXxe9vr0=vr0=LqpWqaaeaabiGaaiaacaqabeaabeqacmaaaOqaaiabicdaWiabc6caUiabigdaXiabiIda4iabiwda1iabgglaXkabicdaWiabc6caUiabicdaWiabisda0iabikdaYmaaDaaaleaacqGHsislcqaIWaamcqGGUaGlcqaIWaamcqaI1aqncqaI3aWnaeaacqGHRaWkcqaIWaamcqGGUaGlcqaIWaamcqaIYaGmcqaIYaGmaaaaaa@4197@
5–50 10 1.152 ± 0.011 0.006 + 0.006 MathType@MTEF@5@5@+=feaafiart1ev1aaatCvAUfKttLearuWrP9MDH5MBPbIqV92AaeXatLxBI9gBaebbnrfifHhDYfgasaacH8bkY=wiFfYlOipiY=Hhbbf9v8qqaqFr0xc9vqpe0di9q8qqpG0dHiVcFbIOFHK8Feei0lXdar=Jb9qqFfeaYRXxe9vr0=vr0=LqpWqaaeaabiGaaiaacaqabeaabeqacmaaaOqaaiabigdaXiabc6caUiabigdaXiabiwda1iabikdaYiabgglaXkabicdaWiabc6caUiabicdaWiabigdaXiabigdaXmaaDaaaleaacqGHsislcqaIWaamcqGGUaGlcqaIWaamcqaIWaamcqaI2aGnaeaacqGHRaWkcqaIWaamcqGGUaGlcqaIWaamcqaIWaamcqaI2aGnaaaaaa@417D@ 0.114 ± 0.043 0.024 + 0.026 MathType@MTEF@5@5@+=feaafiart1ev1aaatCvAUfKttLearuWrP9MDH5MBPbIqV92AaeXatLxBI9gBaebbnrfifHhDYfgasaacH8bkY=wiFfYlOipiY=Hhbbf9v8qqaqFr0xc9vqpe0di9q8qqpG0dHiVcFbIOFHK8Feei0lXdar=Jb9qqFfeaYRXxe9vr0=vr0=LqpWqaaeaabiGaaiaacaqabeaabeqacmaaaOqaaiabicdaWiabc6caUiabigdaXiabigdaXiabisda0iabgglaXkabicdaWiabc6caUiabicdaWiabisda0iabiodaZmaaDaaaleaacqGHsislcqaIWaamcqGGUaGlcqaIWaamcqaIYaGmcqaI0aanaeaacqGHRaWkcqaIWaamcqGGUaGlcqaIWaamcqaIYaGmcqaI2aGnaaaaaa@4185@