2019
DOI: 10.1103/physrevd.99.093008
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Limits on R -parity-violating couplings from Drell-Yan processes at the LHC

Abstract: We find constraints on R-Parity Violating (RPV) couplings of the minimal supersymmetric standard model, using Drell-Yan differential cross sections at the LHC. Specifically, we look at the constraints on λ LQD c couplings from monolepton and dilepton data published by ATLAS, with either electrons or muons in the final state. Out of the 18 RPV couplings to which the LHC is at least potentially sensitive by this technique, we find new limits on 12 (or 13) of them, for squarks masses above 1 (or 2) TeV. We also s… Show more

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Cited by 11 publications
(17 citation statements)
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“…where heref =b,τ , Nb c = 3, Nτ c = 1, m 2 b = mb 1 · mb 2 and m 2 τ = mτ 2 · mτ 3 and it is understood that mτ 2 and mτ 3 are the masses of the two lightest slepton states (τ 1 being the massless Goldstone boson). space is given in [46] and bounds on the TRPV couplings can be found in [60,105].…”
Section: Bilinear Rpv -Numerical Resultsmentioning
confidence: 99%
“…where heref =b,τ , Nb c = 3, Nτ c = 1, m 2 b = mb 1 · mb 2 and m 2 τ = mτ 2 · mτ 3 and it is understood that mτ 2 and mτ 3 are the masses of the two lightest slepton states (τ 1 being the massless Goldstone boson). space is given in [46] and bounds on the TRPV couplings can be found in [60,105].…”
Section: Bilinear Rpv -Numerical Resultsmentioning
confidence: 99%
“…λ 232 < 0.66 mf 1 TeV + 0.42 (18) replace the bounds from DY data in Ref. [2] as the strongest currently available bounds on these two couplings.…”
Section: Electroweak Constraintsmentioning
confidence: 95%
“…One may expect that the effect of one-loop diagrams with O( TeV) sfermion masses would be negligible at the Z-pole. But it has long been known (e.g., [16][17][18]) that the contribution of these diagrams with t-quarks in the loop can be fairly large. This is the result of helicity flips on the t-quark lines.…”
Section: Electroweak Constraintsmentioning
confidence: 99%
See 1 more Smart Citation
“…A simple way to preserve the Higgs naturalness by evading the current experimental constraints is by allowing R-parity Violation (RPV) [11] in the production and decays of superpartners at the LHC. Apart from significantly lowering the collider bounds on the SUSY spectrum [12][13][14][15][16][17][18][19][20][21], RPV SUSY implies the violation of baryon and/or lepton numbers, which has important phenomenological consequences [11].…”
Section: Introductionmentioning
confidence: 99%