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Signal-background interference in gg --> H --> VV

Nikolas Kauer

TL;DR

The paper investigates resonance-continuum interference between the gluon-fusion Higgs signal $gg\rightarrow H\rightarrow VV$ and the continuum background $gg\rightarrow VV$ for a heavy Higgs with $M_H=400$ GeV at the LHC. Using leading-order calculations with leptonic decays and realistic selection cuts via the gg2WW and gg2ZZ tools, the authors quantify interference with measurable metrics $R_1$ and $R_2$ across $\sqrt{s}=7$ and 14 TeV. They find interference effects can reach ~5% at 7 TeV and approach ~10% at 14 TeV, with the size and sign of interference depending on the final state and applied cuts; specific ZZ cuts can suppress interference to about 1%. The results underscore that interference is non-negligible and can be enhanced by selective cuts, signaling that it must be accounted for in LHC Higgs analyses and searches for heavy resonances.

Abstract

The resonance-continuum interference between the SM Higgs search signal process gg --> H --> VV (V=W,Z) and the irreducible background process gg --> VV is studied at leading order for integrated cross sections and differential distributions in pp collisions at \sqrt{s}=7 TeV and 14 TeV for M_H=400 GeV. Leptonic weak boson decays are included, and realistic experimental selection cuts are applied.

Signal-background interference in gg --> H --> VV

TL;DR

The paper investigates resonance-continuum interference between the gluon-fusion Higgs signal and the continuum background for a heavy Higgs with GeV at the LHC. Using leading-order calculations with leptonic decays and realistic selection cuts via the gg2WW and gg2ZZ tools, the authors quantify interference with measurable metrics and across and 14 TeV. They find interference effects can reach ~5% at 7 TeV and approach ~10% at 14 TeV, with the size and sign of interference depending on the final state and applied cuts; specific ZZ cuts can suppress interference to about 1%. The results underscore that interference is non-negligible and can be enhanced by selective cuts, signaling that it must be accounted for in LHC Higgs analyses and searches for heavy resonances.

Abstract

The resonance-continuum interference between the SM Higgs search signal process gg --> H --> VV (V=W,Z) and the irreducible background process gg --> VV is studied at leading order for integrated cross sections and differential distributions in pp collisions at \sqrt{s}=7 TeV and 14 TeV for M_H=400 GeV. Leptonic weak boson decays are included, and realistic experimental selection cuts are applied.

Paper Structure

This paper contains 4 sections, 6 figures, 1 table.

Figures (6)

  • Figure 1: Representative Feynman graphs for the Higgs signal process (left) and the $q\bar{q}$- (centre) and $gg$-initiated (right) continuum background processes at LO.
  • Figure 2: Representative triangle graphs that formally contribute to gluon-induced $VV$ continuum production and decay.
  • Figure 3: Differential cross section distributions for $gg\ (\to H)\to W^-W^+\to l\bar{\nu}_l\bar{l'}\nu_{l'}$ in $pp$ collisions at $\sqrt{s} = 7$ TeV for $M_H=400$ GeV and a single lepton flavour combination calculated at LO. The $p_{Tl}$ [GeV] (left) and $\eta_l$ (right) distributions are shown. Standard cuts are applied (see main text). fb is used as cross section unit.
  • Figure 4: $p_{Tl,\text{min}}$ [GeV] (left) and $p_{Tl,\text{max}}$ [GeV] (right) distributions. Other details as in Fig. \ref{['fig:WW1']}.
  • Figure 5: $M_{l\bar{l'}}$ [GeV] (left) and $\Delta\phi_{l\bar{l'}}$ [$^\circ$] (right) distributions. Other details as in Fig. \ref{['fig:WW1']}.
  • ...and 1 more figures