Limits...
Measurement of electroweak production of two jets in association with a Z boson in proton-proton collisions at [Formula: see text].

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Francis B, Goodell J, Hirosky R, Ledovskoy A, Li H, Lin C, Neu C, Wood J, Clarke C, Harr R, Karchin PE, Kottachchi Kankanamge Don C, Lamichhane P, Sturdy J, Belknap DA, Carlsmith D, Cepeda M, Dasu S, Dodd L, Duric S, Friis E, Hall-Wilton R, Herndon M, Hervé A, Klabbers P, Lanaro A, Lazaridis C, Levine A, Loveless R, Mohapatra A, Ojalvo I, Perry T, Pierro GA, Polese G, Ross I, Sarangi T, Savin A, Smith WH, Vuosalo C, Woods N - Eur Phys J C Part Fields (2015)

Bottom Line: The purely electroweak (EW) cross section for the production of two jets in association with a Z boson, in proton-proton collisions at [Formula: see text], is measured using data recorded by the CMS experiment at the CERN LHC, corresponding to an integrated luminosity of 19.7[Formula: see text].The electroweak cross section for the [Formula: see text] final state (with [Formula: see text] or [Formula: see text] and j representing the quarks produced in the hard interaction) in the kinematic region defined by [Formula: see text][Formula: see text], [Formula: see text][Formula: see text], transverse momentum [Formula: see text][Formula: see text], and pseudorapidity [Formula: see text], is found to be [Formula: see text], in agreement with the standard model prediction.The associated jet activity of the selected events is studied, in particular in a signal-enriched region of phase space, and the measurements are found to be in agreement with QCD predictions.

View Article: PubMed Central - PubMed

Affiliation: Yerevan Physics Institute, Yerevan, Armenia.

ABSTRACT

The purely electroweak (EW) cross section for the production of two jets in association with a Z boson, in proton-proton collisions at [Formula: see text], is measured using data recorded by the CMS experiment at the CERN LHC, corresponding to an integrated luminosity of 19.7[Formula: see text]. The electroweak cross section for the [Formula: see text] final state (with [Formula: see text] or [Formula: see text] and j representing the quarks produced in the hard interaction) in the kinematic region defined by [Formula: see text][Formula: see text], [Formula: see text][Formula: see text], transverse momentum [Formula: see text][Formula: see text], and pseudorapidity [Formula: see text], is found to be [Formula: see text], in agreement with the standard model prediction. The associated jet activity of the selected events is studied, in particular in a signal-enriched region of phase space, and the measurements are found to be in agreement with QCD predictions.

No MeSH data available.


Related in: MedlinePlus

Distributions for the BDT discriminants in  events, for the control region (top row) and signal region (bottom row), used by analysis B. The ratio for data to MC simulations is given in the bottom panel on the left, showing the impact of changes in JES by 1 SD. The bottom panel on the right shows the difference between data or the expected  contribution with respect to the background (BG)
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Fig8: Distributions for the BDT discriminants in events, for the control region (top row) and signal region (bottom row), used by analysis B. The ratio for data to MC simulations is given in the bottom panel on the left, showing the impact of changes in JES by 1 SD. The bottom panel on the right shows the difference between data or the expected contribution with respect to the background (BG)

Mentions: Figures 7, 8 and 9 show the distributions of the discriminants for the three analyses. Good agreement is observed overall in both the signal and in the control regions which are defined according to the value of the or variables (see Sect. 5.3).Fig. 9


Measurement of electroweak production of two jets in association with a Z boson in proton-proton collisions at [Formula: see text].

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Distributions for the BDT discriminants in  events, for the control region (top row) and signal region (bottom row), used by analysis B. The ratio for data to MC simulations is given in the bottom panel on the left, showing the impact of changes in JES by 1 SD. The bottom panel on the right shows the difference between data or the expected  contribution with respect to the background (BG)
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Fig8: Distributions for the BDT discriminants in events, for the control region (top row) and signal region (bottom row), used by analysis B. The ratio for data to MC simulations is given in the bottom panel on the left, showing the impact of changes in JES by 1 SD. The bottom panel on the right shows the difference between data or the expected contribution with respect to the background (BG)
Mentions: Figures 7, 8 and 9 show the distributions of the discriminants for the three analyses. Good agreement is observed overall in both the signal and in the control regions which are defined according to the value of the or variables (see Sect. 5.3).Fig. 9

Bottom Line: The purely electroweak (EW) cross section for the production of two jets in association with a Z boson, in proton-proton collisions at [Formula: see text], is measured using data recorded by the CMS experiment at the CERN LHC, corresponding to an integrated luminosity of 19.7[Formula: see text].The electroweak cross section for the [Formula: see text] final state (with [Formula: see text] or [Formula: see text] and j representing the quarks produced in the hard interaction) in the kinematic region defined by [Formula: see text][Formula: see text], [Formula: see text][Formula: see text], transverse momentum [Formula: see text][Formula: see text], and pseudorapidity [Formula: see text], is found to be [Formula: see text], in agreement with the standard model prediction.The associated jet activity of the selected events is studied, in particular in a signal-enriched region of phase space, and the measurements are found to be in agreement with QCD predictions.

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Affiliation: Yerevan Physics Institute, Yerevan, Armenia.

ABSTRACT

The purely electroweak (EW) cross section for the production of two jets in association with a Z boson, in proton-proton collisions at [Formula: see text], is measured using data recorded by the CMS experiment at the CERN LHC, corresponding to an integrated luminosity of 19.7[Formula: see text]. The electroweak cross section for the [Formula: see text] final state (with [Formula: see text] or [Formula: see text] and j representing the quarks produced in the hard interaction) in the kinematic region defined by [Formula: see text][Formula: see text], [Formula: see text][Formula: see text], transverse momentum [Formula: see text][Formula: see text], and pseudorapidity [Formula: see text], is found to be [Formula: see text], in agreement with the standard model prediction. The associated jet activity of the selected events is studied, in particular in a signal-enriched region of phase space, and the measurements are found to be in agreement with QCD predictions.

No MeSH data available.


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