2020
DOI: 10.1140/epjc/s10052-019-7594-6
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Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $$\sqrt{s}=13$$ $$\text {TeV}$$ pp collisions using the ATLAS detector

Abstract: A search for the electroweak production of charginos and sleptons decaying into final states with two electrons or muons is presented. The analysis is based on 139 fb −1 of proton-proton collisions recorded by the ATLAS detector at the Large Hadron Collider at √ s = 13 TeV. Three R-parity-conserving scenarios where the lightest neutralino is the lightest supersymmetric particle are considered: the production of chargino pairs with decays via either W bosons or sleptons, and the direct production of slepton pai… Show more

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Cited by 261 publications
(284 citation statements)
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“…There are two reasons for this. First and foremost, multi-lepton searches at the LHC via Drell-Yan production constrain the particles carrying SU(2) L ×U(1) Y quantum numbers to masses above the 400−600 GeV range [53][54][55]. On the other hand, if one were to roughly extrapolate a similar reasoning to m 1 , m 2 , m 3 smaller than the mass of the muon, so that the corresponding particles may possibly result invisible at the LHC, these would still necessarily contribute at one loop to the anomalous magnetic moment of the muon.…”
Section: Jhep08(2020)148mentioning
confidence: 99%
“…There are two reasons for this. First and foremost, multi-lepton searches at the LHC via Drell-Yan production constrain the particles carrying SU(2) L ×U(1) Y quantum numbers to masses above the 400−600 GeV range [53][54][55]. On the other hand, if one were to roughly extrapolate a similar reasoning to m 1 , m 2 , m 3 smaller than the mass of the muon, so that the corresponding particles may possibly result invisible at the LHC, these would still necessarily contribute at one loop to the anomalous magnetic moment of the muon.…”
Section: Jhep08(2020)148mentioning
confidence: 99%
“…8 At the LHC there is currently no specific search for particles with the quantum numbers of S and X. However, slepton pair production with their subsequent decays to a lepton plus a neutralino provide the same signal and thus, we can make a reinterpretation of the corresponding searches at CMS [57] and ATLAS [58]. The CMS slepton search [57] is based on 35.9/fb, while ATLAS' chargino and slepton search [58] uses 139/fb.…”
Section: Resultsmentioning
confidence: 99%
“…In the following we are focusing on the simplest topology pp → L + L − → µ + µ − + / E T . The latest available analysis of this signal has been presented by ATLAS in [70] (see also the results with a smaller data set in [71]). The resulting bound on the production cross section can be as strong as σ 0.2 fb (for M L M S 1 ), which corresponds to M L 900 GeV (according to the LO production cross section as calculated by MadGraph5 [67]).…”
Section: Lhc Phenomenologymentioning
confidence: 99%
“…The most sensitive signature is thus again 2 [70] or 3 [72] leptons (from the leptonic decays of the gauge bosons) and / E T . This searches can constrain Higgsino-like charginos and neutralinos with masses up to about 600 GeV.…”
Section: Jhep10(2020)070mentioning
confidence: 99%
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