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Boson fusion and Higgs production at the CERN LHC in six fermion final states with one charged lepton pair

Elena Accomando, Alessandro Ballestrero, Aissa Belhouari, and Ezio Maina
Phys. Rev. D 75, 113006 – Published 20 June 2007

Abstract

Boson boson scattering and Higgs production in boson boson fusion will be actively investigated at the CERN LHC. We have performed a parton level study of all processes of the type q1q2q3q4q5q6l+l using for the first time a full fledged six fermion Monte Carlo event generator which employs exact matrix elements at O(αem6). We have examined Higgs production in vector boson fusion followed by the decay chain HZZl+ljj, including exactly all electroweak irreducible backgrounds. In the high mass region we have compared the case of a relatively light Higgs with the no-Higgs results. The integrated cross section for the latter case is more than twice that in the former for a minimum invariant mass of the ZV pair of about 800 GeV. We find, in a preliminary analysis at parton level, that, summing up the muon and the electron channels, about 25 events are expected in the light Higgs case for L=100fb1.

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  • Received 28 September 2006

DOI:https://doi.org/10.1103/PhysRevD.75.113006

©2007 American Physical Society

Authors & Affiliations

Elena Accomando*, Alessandro Ballestrero, Aissa Belhouari, and Ezio Maina§

  • INFN, Sezione di Torino and Dipartimento di Fisica Teorica, Università di Torino, Via Giuria 1, 10125 Torino, Italy

  • *accomand@to.infn.it
  • ballestr@to.infn.it
  • belhouar@to.infn.it
  • §maina@to.infn.it

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Vol. 75, Iss. 11 — 1 June 2007

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Images

  • Figure 1
    Figure 1
    Vector boson fusion processes.Reuse & Permissions
  • Figure 2
    Figure 2
    Examples of EW irreducible background to vector boson scattering processes.Reuse & Permissions
  • Figure 3
    Figure 3
    Higgs boson production via vector boson fusion and Higgsstrahlung.Reuse & Permissions
  • Figure 4
    Figure 4
    Fundamental topologies associated with 4Z processes. Total number of diagrams 2263/1251/803/615/579.Reuse & Permissions
  • Figure 5
    Figure 5
    Decays of the off shell neutral bosons Z, γ, H.Reuse & Permissions
  • Figure 6
    Figure 6
    Invariant mass distribution of the two charged leptons and the two most central quarks, for different sets of processes. The upper plot includes the set of cuts described in the text. In the lower plot a further cut for vetoing top production is applied.Reuse & Permissions
  • Figure 7
    Figure 7
    Distribution of the invariant mass M(VZ) of the two candidate vector bosons for a Higgs mass of 150 GeV and 200 GeV. The contribution of the various subprocesses is evaluated as in Sec. 3.Reuse & Permissions
  • Figure 8
    Figure 8
    Invariant mass distribution for M(VZ)>800GeV. The solid and long-dashed lines refer to the no-Higgs case, the short-dashed and dot-dashed ones to M(H)=200GeV. All results satisfy the standard acceptance cuts. The solid and short-dashed lines present the results for our signal definition. For the long-dashed and dot-dashed histograms, we have further required |η(Zll)|<2 and |η(qV)|<2.Reuse & Permissions
  • Figure 9
    Figure 9
    Pseudorapidity distribution of the lepton pair for the no-Higgs case (solid line) and for M(H)=200GeV (dashed line). All events satisfy M(ZV)>800GeV.Reuse & Permissions
  • Figure 10
    Figure 10
    M(ZZ) (left panel) and M(WZ) (right panel) invariant mass distribution for M(VZ)>800GeV. The solid and long-dashed lines refer to the no-Higgs case, the short-dashed and dot-dashed ones to M(H)=200GeV. The solid and short-dashed lines present the results for our signal definition. For the long-dashed dot-dashed histograms, we have further required |η(Zll)|<2 and |η(qV)|<2.Reuse & Permissions
  • Figure 11
    Figure 11
    Pseudorapidity distribution of the lepton pair in qqZZ (left panel) and qqZW (right panel) final states. The solid line refers to the no-Higgs case, the dashed one to M(H)=200GeV. In all cases M(VZ)>800GeV.Reuse & Permissions
  • Figure 12
    Figure 12
    Invariant mass distribution of the lepton pair and the two jets from boson decay for the no-Higgs case. The solid (dashed) line is obtained by identifying the two most central jets as the vector boson decay products before (after) top vetoing. The dotted line is obtained by requiring the correct flavor content for the jets identified as decay products of both the vector boson and the top. The dot-dashed line is produced using solely invariant mass information to identify the vector boson and the top decay products.Reuse & Permissions
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