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Measurement of the electroweak production of dijets in association with a Z-boson and distributions sensitive to vector boson fusion in proton-proton collisions at $\sqrt{s} =$ 8 TeV using the ATLAS detector

The collaboration
JHEP 1404 (2014) 031, 2014

Abstract (data abstract)
Measurements of cross sections and differential distributions for inclusive Z-boson-plus-dijet production are performed in five fiducial regions, each with different sensitivity to the electroweak contribution. WARNING: a future update will be made with the breakdown of systematic uncertainties. UPDATE (09 JUN 2014): slight correction to systematic uncertainties.

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Data from Fig. 6a

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Unfolded normalised differential Z+2j cross section as a function of dijet invariant mass in the baseline region.

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Data from Fig. 6b

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Unfolded normalised differential Z+2j cross section as a function of dijet invariant mass in the search region.

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Data from Fig. 7a

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Unfolded normalised differential Z+2j cross section as a function of the rapidity separation between the leading jets in the baseline...

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Data from Fig. 7b

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Unfolded normalised differential Z+2j cross section as a function of the rapidity separation between the leading jets in the search...

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Data from Fig. 8a

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Unfolded normalised differential cross section distribution as a function of the number of jets in the rapidity interval between the...

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Data from Fig. 8b

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Unfolded normalised differential cross section distribution as a function of the normalised transverse momentum balance in the high mass region.

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Data from Fig. 8c

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Unfolded normalised differential cross section distribution as a function of the azimuthal angle between the two leading jets in the...

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Data from Fig. 9a

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Unfolded jet veto efficiency as a function of the dijet invariant mass in the baseline region.

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Data from Fig. 9b

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Unfolded jet veto efficiency as a function of the rapidity separation between the two leading jets in the baseline region.

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Data from Fig. 9c

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Unfolded average number of jets in the rapidity interval between the two leading jets as a function of the dijet...

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Data from Fig. 9d

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Unfolded average number of jets in the rapidity interval between the two leading jets as a function of the rapidity...

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Data from Fig. 10a

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Unfolded transverse momentum balance veto efficiency as a function of the dijet invariant mass in the baseline region.

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Data from Fig. 10b

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Unfolded transverse momentum balance veto efficiency as a function of the rapidity separation between the two leading jets in the...

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Data from Figaux. 1a

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Unfolded normalised differential Z+2j cross section as a function of dijet invariant mass in the high-pt region.

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Data from Figaux. 1b

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Unfolded normalised differential Z+2j cross section as a function of dijet invariant mass in the control region.

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Data from Figaux. 2a

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Unfolded normalised differential Z+2j cross section as a function of the rapidity separation between the leading jets in the high-pt...

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Data from Figaux. 2b

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Unfolded normalised differential Z+2j cross section as a function of the rapidity separation between the leading jets in the control...

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Data from Figaux. 3a

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Unfolded jet veto efficiency as a function of the dijet invariant mass in the high-pt region.

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Data from Figaux. 3b

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Unfolded jet veto efficiency as a function of the rapidity separation between the two leading jets in the high-pt region.

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Data from Figaux. 3c

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Unfolded average number of jets in the rapidity interval between the two leading jets as a function of the dijet...

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Data from Figaux. 3d

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Unfolded average number of jets in the rapidity interval between the two leading jets as a function of the rapidity...

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Data from Figaux. 4a

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Unfolded transverse momentum balance veto efficiency as a function of the dijet invariant mass in the high-pt region.

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Data from Figaux. 4b

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Unfolded transverse momentum balance veto efficiency as a function of the rapidity separation between the two leading jets in the...