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Boosting low-mass hadronic resonances

Chase Shimmin and Daniel Whiteson
Phys. Rev. D 94, 055001 – Published 1 September 2016

Abstract

Searches for new hadronic resonances typically focus on high-mass spectra due to overwhelming QCD backgrounds and detector trigger rates. We present a study of searches for relatively low-mass hadronic resonances at the LHC in the case that the resonance is boosted by recoiling against a well-measured high-pT probe such as a muon, photon or jet. The hadronic decay of the resonance is then reconstructed either as a single large-radius jet or as a resolved pair of standard narrow-radius jets, balanced in transverse momentum to the probe. We show that the existing 2015 LHC data set of pp collisions with Ldt=4fb1 should already have powerful sensitivity to a generic Z model which couples only to quarks, for Z masses ranging from 20500GeV/c2.

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  • Received 2 June 2016

DOI:https://doi.org/10.1103/PhysRevD.94.055001

© 2016 American Physical Society

Physics Subject Headings (PhySH)

Particles & Fields

Authors & Affiliations

Chase Shimmin and Daniel Whiteson

  • Department of Physics and Astronomy, UC Irvine, Irvine, California 92627

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Issue

Vol. 94, Iss. 5 — 1 September 2016

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Images

  • Figure 1
    Figure 1

    Diagrams of Z production with recoil against either a gluon (top), a photon or W boson (botton).

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  • Figure 2
    Figure 2

    Production cross sections at s=13TeV in pp collisions for j+Z, W+Z and γ+Z. Also shown is the width of the Z as a function of mass for several choices of gauge coupling gB. All calculations include the parton-level requirement of a jet, charged lepton, or photon in their respective channels with pT>10GeV.

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  • Figure 3
    Figure 3

    Distribution at s=13TeV and Ldt=4fb1 of reconstructed Z candidate mass in the γ+Z channel, for both the single large-R jet (top) and the resolved dijet case (bottom) considered in the text. Also shown are signal distributions, generated with gB=1.5, and scaled by a factor of 10 for visibility.

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  • Figure 4
    Figure 4

    Distribution at s=13TeV and Ldt=4fb1 of reconstructed Z candidate mass in the W(μν)+Z channel, for both the single large-R jet (top) and the resolved dijet case (bottom) considered in the text. Also shown are signal distributions, generated with gB=1.5, and scaled by a factor of 10 for visibility.

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  • Figure 5
    Figure 5

    Distribution at s=13TeV and Ldt=4fb1 of reconstructed Z candidate mass in the jet+Z channel, for both the single large-R jet (top) and the resolved dijet case (bottom) considered in the text. Also shown are signal distributions, generated with gB=1.5, and scaled by a factor 50 for visibility.

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  • Figure 6
    Figure 6

    Expected upper limits at 95% C.L. on the coupling gB between the hypothetical Z boson and quarks, for the γ+Z, W+Z, and jet+Z channels, in both the single large-R jet as well as the dijet modes, for values of MZ from 20–500 GeV. If the k factors for the largest backgrounds are doubled, the limits are weakened by 17%–21%. The limits are calculated for the case of pp collisions at s=13TeV with Ldt=4fb1. For comparison, we include existing limits from UA2 and CDF (shaded contours), as interpreted by [1].

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