Abstract

The associated production of a single-top with opposite-sign same-flavor (OSSF) di-leptons, $pp \to t \ell^+ \ell^-$ and $ pp \to t \ell^+ \ell^- + j$ ($j=$light jet), can lead to striking tri-lepton $pp \to \ell^\prime \ell^+ \ell^- + X$ and di-lepton $pp \to \ell^+ \ell^- + j_b + X$ ($j_b=b$-jet) events at the LHC, after the top decays. Although these rather generic multi-lepton signals are flavor-blind, they can be generated by new 4-Fermi flavor changing (FC) $u_i t \ell \ell$ scalar, vector and tensor interactions ($u_i \in u,c$), which we study in this paper; we match the FC $u_i t \ell \ell$ 4-Fermi terms to the SMEFT operators and also to different types of FC underlying heavy physics. The main backgrounds to these di- and tri-lepton signals arise from $t \bar t$, $Z$+jets and $VV$ ($V=W,Z$) production, but they can be essentially eliminated with a sufficiently high invariant mass selection on the OSSF di-leptons, $m_{\ell^+ \ell^-}^{\tt min}(OSSF) > 1$ TeV; the use of $b$-tagging as an additional selection in the di-lepton final state case also proves very useful. We find, for example, that the expected 95\% CL bounds on the scale of a tensor(vector) $u t \mu \mu$ interaction, with the current $\sim 140$ fb$^{-1}$ of LHC data, are $\Lambda < 5(3.2) $ TeV or $\Lambda < 4.1(2.7)$ TeV, if analyzed via the di-muon $\mu^+ \mu^- + j_b$ signal or the $e \mu^+ \mu^-$ tri-lepton one, respectively. The expected reach at the HL-LHC with 3000 fb$^{-1}$ of data is $\Lambda < 7.1(4.7)$ TeV and $\Lambda < 2.4(1.5)$ TeV for the corresponding $u t \mu \mu$ and $c t \mu \mu$ operators. We also study the potential sensitivity at future 27 TeV and 100 TeV high-energy LHC successors and also discuss the possible implications of this class of FC 4-Fermi effective interactions on lepton non-universality tests at the LHC.

Highlights

  • The origin of the observed flavor pattern in the fermion sector still remains one of the fundamental unresolved questions in theoretical particle physics

  • Heavy physics containing e.g., heavy scalars and/or vectors. We showed that these higher-dimensional flavor-changing neutral currents (FCNC) top interactions can lead to new single-top þ dilepton signals at the LHC via pp → tlþl− and pp → tlþl− þ j (j 1⁄4 light jet), which can be efficiently probed via the dilepton þ b-jet pp → lþl− þ jb þ X signal and/or in trilepton pp → l0lþl− þ X events, containing oppositesign same-flavor (OSSF) dileptons, e.g., pp → eμþμ− þ X, if the new physics (NP) involves the tuiμμ contact terms and the top decays via t → bW → beνe

  • We have studied in some detail the Standard Model (SM) background to these di- and trilepton signatures, which is dominated by pp → tt; Z þ jets; WZ and showed that an excellent separation between the NP signals and the background can be obtained with a selection of events with high opposite-sign same-flavor (OSSF)

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Summary

INTRODUCTION

The origin of the observed flavor pattern in the fermion sector still remains one of the fundamental unresolved questions in theoretical particle physics. The ðtllÞ1 channel pp → tlþl−j does have potentially significant SM contributions [78,79,80,81,82], which is dominated by the EW associated production of a single-top with a Z-boson and an accompanying light-jet, i.e., via ub → tZj in the five-flavor scheme, followed by the decay Z → lþl− as shown in the left diagram of Fig. 1. In terms of the coefficients of the effective operators, the vectorlike (Vlij), scalarlike (Slij), and tensorlike (Tlij) couplings are given by (we henceforward drop the superscript l): VLL 1⁄4 αðl1qÞ − αðl3qÞ; VLR 1⁄4 αlu; VRR 1⁄4 αeu; VRL 1⁄4 αqe; SRR 1⁄4 −αðl1eÞqu; SLL 1⁄4 SLR 1⁄4 SRL 1⁄4 0; TRR 1⁄4 −αðl3eÞqu; TLL 1⁄4 TLR 1⁄4 TRL 1⁄4 0: ð6Þ These 4-Fermi interactions can be generated through tree-level exchanges of heavy vectors and scalars in the underlying heavy theory (or their Fierz transforms). Note that no LL tensor or LL, LR and RL scalar terms are generated at dimension 6; they can, be generated by dimension 8 operators and have coefficients suppressed by ∼ðv2=Λ4Þ, where v 1⁄4 246 GeV is the Higgs vacuum expectation value

Examples of matching to underlying beyond the SM scenarios
The tuiee 4-Fermi operators involving two electrons
The tuiμμ 4-Fermi operators involving two muons
Implications of gauge invariance
SIGNAL AND BACKGROUND ANALYSIS
Event selection: signal vs background
Domain of validity of the EFT setup
Sensitivity to the NP
A MORE REALISTIC STUDY
Simulated event samples
Event selection
Results
LEPTON FLAVOR NONUNIVERSALITY
SUMMARY
Full Text
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