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[PDF] Top 20 Searches for $R$-parity-violating supersymmetry in $pp $collisions at $\sqrt(s) =$ 8 TeV in final states with 0-4 leptons

Has 10000 "Searches for $R$-parity-violating supersymmetry in $pp $collisions at $\sqrt(s) =$ 8 TeV in final states with 0-4 leptons" found on our website. Below are the top 20 most common "Searches for $R$-parity-violating supersymmetry in $pp $collisions at $\sqrt(s) =$ 8 TeV in final states with 0-4 leptons".

Searches for $R$-parity-violating supersymmetry in $pp $collisions at $\sqrt(s) =$ 8 TeV in final states with 0-4 leptons

Searches for $R$-parity-violating supersymmetry in $pp $collisions at $\sqrt(s) =$ 8 TeV in final states with 0-4 leptons

... Studies in Theoretical Physics and Mathematics, Iran; the Science Foundation, Ireland; the Istituto Nazionale di Fisica Nucleare, Italy; the Ministry of Science, ICT and Future Planning, and National Research ... See full document

66

Search for $R$-parity violating supersymmetry in pp collisions at $\sqrt{s} = $ 13 TeV using b jets in a final state with a single lepton, many jets, and high sum of large-radius jet masses

Search for $R$-parity violating supersymmetry in pp collisions at $\sqrt{s} = $ 13 TeV using b jets in a final state with a single lepton, many jets, and high sum of large-radius jet masses

... data at a center-of-mass energy of √ s = 13 TeV corresponding to an inte- grated luminosity of ...embedded in the magnetic flux- return yoke outside the ...together with a definition of the ... See full document

26

Searches for pair production of charginos and top squarks in final states with two oppositely charged leptons in proton-proton collisions at $\sqrt{s}=$ 13 TeV

Searches for pair production of charginos and top squarks in final states with two oppositely charged leptons in proton-proton collisions at $\sqrt{s}=$ 13 TeV

... phenomena with outstanding ...[3–5]. Supersymmetry [6–14] is an extension of the SM that assigns a fermion (boson) superpartner to every SM boson ...if R-parity [18] is conserved, the lightest ... See full document

49

A search for top squarks with R-parity-violating decays to all-hadronic final states with the ATLAS detector in $\sqrt{s}$ = 8 TeV proton-proton collisions

A search for top squarks with R-parity-violating decays to all-hadronic final states with the ATLAS detector in $\sqrt{s}$ = 8 TeV proton-proton collisions

... differences in response to hadrons compared to electrons, signal losses due to noise-suppression threshold e ffects, and energy lost in non-instrumented ...The final jet energy calibration is derived ... See full document

46

Search for supersymmetry at $\sqrt{s}=13$  TeV in final states with jets and two same-sign leptons or three leptons with the ATLAS detector

Search for supersymmetry at $\sqrt{s}=13$  TeV in final states with jets and two same-sign leptons or three leptons with the ATLAS detector

... SUSY in final states with two leptons (electrons or muons) of the same electric charge (referred to as same-sign (SS) leptons) [ 22 ] or three leptons (3L) in any ... See full document

38

Search for anomalous production of events with three or more leptons in $pp$ collisions at $\sqrt(s) =$ 8 TeV

Search for anomalous production of events with three or more leptons in $pp$ collisions at $\sqrt(s) =$ 8 TeV

... [1–3] at the relatively low mass of about 125 GeV implies that physics beyond the standard model (BSM) may be observable at energy scales of around 1 ...TeV. Supersymmetry (SUSY) is a ... See full document

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Search for R-parity violating decays of a top squark in proton-proton collisions at $\sqrt{s}$ = 8 TeV

Search for R-parity violating decays of a top squark in proton-proton collisions at $\sqrt{s}$ = 8 TeV

... containing leptons, we im- pose isolation constraints on the transverse energy E T , cone from charged-particle tracks or deposits in the calorimeter within a cone  R =  ( η ) 2 + (φ) 2 = ... See full document

24

Searches for supersymmetry based on events with b jets and four W bosons in pp collisions at 8 TeV

Searches for supersymmetry based on events with b jets and four W bosons in pp collisions at 8 TeV

... 28] with four W ...the final states contain 04 ...the final states with different lepton multiplicities ...the leptons, providing five mutually exclusive ... See full document

35

Search for direct top squark pair production in final states with two tau leptons in pp collisions at $\sqrt{s}=8$  TeV with the ATLAS detector

Search for direct top squark pair production in final states with two tau leptons in pp collisions at $\sqrt{s}=8$  TeV with the ATLAS detector

... shape in the calorimeters and information from the tracking system are used to separate the collimated τ had decay products from the generally broader jets resulting from quark and gluon ...contained in a ... See full document

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Search for electroweak production of charginos in final states with two τ leptons in pp collisions at $ \sqrt{s}=8 $ TeV

Search for electroweak production of charginos in final states with two τ leptons in pp collisions at $ \sqrt{s}=8 $ TeV

... χ 0 ), and sleptons (e ` ) by the ATLAS and CMS Collabo- rations are described in ...[14–20]. In various SUSY models, the lightest SUSY partners of the SM leptons are those of the third ... See full document

46

Search for supersymmetry in hadronic final states with missing transverse energy using the variables $\alpha_T$ and b-quark multiplicity in pp collisions at $\sqrt s=8$ TeV

Search for supersymmetry in hadronic final states with missing transverse energy using the variables $\alpha_T$ and b-quark multiplicity in pp collisions at $\sqrt s=8$ TeV

... e.g. at the TeV scale, is motivated by the cancellation of the quadratically divergent loop corrections to the Higgs boson mass in the SM [7, ...8]. In order to avoid a large amount of ... See full document

45

Searches for third-generation squark production in fully hadronic final states in proton-proton collisions at $ \sqrt{s} = 8$ TeV

Searches for third-generation squark production in fully hadronic final states in proton-proton collisions at $ \sqrt{s} = 8$ TeV

... survive with a modest amount of fine tuning if sparticles are not much heavier than their SM ...particles in particular, the mass difference between a particle and its corresponding sparticle should not be ... See full document

61

Search for R-parity violating supersymmetry with displaced vertices in proton-proton collisions at $\sqrt{s}$ = 8 TeV

Search for R-parity violating supersymmetry with displaced vertices in proton-proton collisions at $\sqrt{s}$ = 8 TeV

... for R-parity violating supersymmetry in proton-proton collision events collected by the CMS experiment at a center-of-mass energy of p ffiffiffi s ¼ 8 ...flavor violating ... See full document

23

Search for R-parity-violating supersymmetry in events with four or more leptons in $\sqrt{s}=7$ TeV $pp$ collisions with the ATLAS detector

Search for R-parity-violating supersymmetry in events with four or more leptons in $\sqrt{s}=7$ TeV $pp$ collisions with the ATLAS detector

... each with spin (S) dif- fering by one-half unit from that of its SM ...introduced in SUSY models can violate the conservation of baryon (B) and lepton (L) number and lead to a proton lifetime shorter than ... See full document

41

Searches for light- and heavy-flavour three-jet resonances in pp collisions at $\sqrt{s} = 8$ TeV

Searches for light- and heavy-flavour three-jet resonances in pp collisions at $\sqrt{s} = 8$ TeV

... multijet final states at hadron colliders offer a unique window on many possible extensions of the standard model (SM), although with the view partly obscured by large back- grounds due to SM ... See full document

33

Search for stealth supersymmetry in events with jets, either photons or leptons, and low missing transverse momentum in pp collisions at 8 TeV

Search for stealth supersymmetry in events with jets, either photons or leptons, and low missing transverse momentum in pp collisions at 8 TeV

... SUSY with low ~ p miss T final states, the so-called stealth scenario [22, 23] has received relatively little ...particles at the weak scale, analogous to the SUSY-breaking sector, which ... See full document

35

Search for supersymmetry in events with a photon, a lepton, and missing transverse momentum in pp collisions at $\sqrt s=$ 8 TeV

Search for supersymmetry in events with a photon, a lepton, and missing transverse momentum in pp collisions at $\sqrt s=$ 8 TeV

... accommodated in the SM, such as the existence of dark mat- ter in the universe or the extreme fine tuning required to control radiative corrections to the Higgs boson mass (hierarchy problem) ...framework ... See full document

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Search for natural supersymmetry in events with top quark pairs and photons in pp collisions at $\sqrt{s} =$ 8 TeV

Search for natural supersymmetry in events with top quark pairs and photons in pp collisions at $\sqrt{s} =$ 8 TeV

... peak at the Z boson mass in the invariant mass distribution of electron-photon pairs in the electron+jets channel of ...bosons in the electron+jets channel, the accuracy of which can be ... See full document

36

Phenomenological MSSM interpretation of CMS searches in pp collisions at sqrt(s) = 7 and 8 TeV

Phenomenological MSSM interpretation of CMS searches in pp collisions at sqrt(s) = 7 and 8 TeV

... Studies in Theoretical Physics and Mathematics, Iran; the Science Foundation, Ireland; the Istituto Nazionale di Fisica Nucleare, Italy; the Ministry of Science, ICT and Future Planning, and National Research ... See full document

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Search for Supersymmetry Using Razor Variables in Events with $b$-Tagged Jets in $pp$ Collisions at $\sqrt{s} =$ 8 TeV

Search for Supersymmetry Using Razor Variables in Events with $b$-Tagged Jets in $pp$ Collisions at $\sqrt{s} =$ 8 TeV

... particle at the electroweak scale are well motivated because they may explain the origin of dark ...[10–12] at the CERN LHC has renewed interest in “natural” SUSY models, which minimize the ... See full document

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