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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 ATLAS 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.

  • Table 1

    Data from Fig. 6a

    10.17182/hepdata.62729.v1/t1

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

  • Table 2

    Data from Fig. 6b

    10.17182/hepdata.62729.v1/t2

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

  • Table 3

    Data from Fig. 7a

    10.17182/hepdata.62729.v1/t3

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

  • Table 4

    Data from Fig. 7b

    10.17182/hepdata.62729.v1/t4

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

  • Table 5

    Data from Fig. 8a

    10.17182/hepdata.62729.v1/t5

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

  • Table 6

    Data from Fig. 8b

    10.17182/hepdata.62729.v1/t6

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

  • Table 7

    Data from Fig. 8c

    10.17182/hepdata.62729.v1/t7

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

  • Table 8

    Data from Fig. 9a

    10.17182/hepdata.62729.v1/t8

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

  • Table 9

    Data from Fig. 9b

    10.17182/hepdata.62729.v1/t9

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

  • Table 10

    Data from Fig. 9c

    10.17182/hepdata.62729.v1/t10

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

  • Table 11

    Data from Fig. 9d

    10.17182/hepdata.62729.v1/t11

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

  • Table 12

    Data from Fig. 10a

    10.17182/hepdata.62729.v1/t12

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

  • Table 13

    Data from Fig. 10b

    10.17182/hepdata.62729.v1/t13

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

  • Table 14

    Data from Figaux. 1a

    10.17182/hepdata.62729.v1/t14

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

  • Table 15

    Data from Figaux. 1b

    10.17182/hepdata.62729.v1/t15

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

  • Table 16

    Data from Figaux. 2a

    10.17182/hepdata.62729.v1/t16

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

  • Table 17

    Data from Figaux. 2b

    10.17182/hepdata.62729.v1/t17

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

  • Table 18

    Data from Figaux. 3a

    10.17182/hepdata.62729.v1/t18

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

  • Table 19

    Data from Figaux. 3b

    10.17182/hepdata.62729.v1/t19

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

  • Table 20

    Data from Figaux. 3c

    10.17182/hepdata.62729.v1/t20

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

  • Table 21

    Data from Figaux. 3d

    10.17182/hepdata.62729.v1/t21

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

  • Table 22

    Data from Figaux. 4a

    10.17182/hepdata.62729.v1/t22

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

  • Table 23

    Data from Figaux. 4b

    10.17182/hepdata.62729.v1/t23

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

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