[PDF] Top 20 Limits on anomalous trilinear gauge couplings from WW -> e(+)e(-), WW -> e(+/-)mu(-/+), and WW ->mu(+)mu(-) events from pp collisions at root s=1.96 TeV
Has 10000 "Limits on anomalous trilinear gauge couplings from WW -> e(+)e(-), WW -> e(+/-)mu(-/+), and WW ->mu(+)mu(-) events from pp collisions at root s=1.96 TeV" found on our website. Below are the top 20 most common "Limits on anomalous trilinear gauge couplings from WW -> e(+)e(-), WW -> e(+/-)mu(-/+), and WW ->mu(+)mu(-) events from pp collisions at root s=1.96 TeV".
Limits on anomalous trilinear gauge couplings from WW -> e(+)e(-), WW -> e(+/-)mu(-/+), and WW ->mu(+)mu(-) events from pp collisions at root s=1.96 TeV
... P. Banerjee, 29 S. Banerjee, 29 E. Barberis, 64 P. Bargassa, 81 P. Baringer, 59 C. Barnes, 44 J. Barreto, 2 J. F. Bartlett, 51 U. Bassler, 17 D. Bauer, 44 A. Bean, 59 M. Begalli, 3 M. Begel, 72 C. ... See full document
6
Measurement of the ${{\mathrm{W} }^{+} }\mathrm{W}^{-} $ cross section in pp collisions at $\sqrt{s} =$ 8 TeV and limits on anomalous gauge couplings
... lisions at √ s = 8 TeV is ...detector at the LHC correspond to an integrated luminosity of ...− 1 . The W + W − candidates are selected from events with two charged ... See full document
44
Production of WZ events in pp(-) collisions at root s=1.96 TeV and limits on anomalous WWZ couplings
... requires at least three charged leptons that originate from a common interaction vertex and survive the electron or muon identification criteria outlined ...bosons and suppress backgrounds ... See full document
7
Evidence of WW and WZ Production with lepton plus jets Final States in pp Collisions at root s=1.96 TeV
... ¼ 1:96 GeV predicted by the SM are ðWWÞ ¼ 12:4 0:8 pb and ðWZÞ ¼ 3:7 0:3 pb ...originating from anoma- lous trilinear gauge boson couplings ...of WW ... See full document
7
Study Z gamma events and limits on anomalous ZZ gamma and Z gamma gamma couplings in pp(-) collisions at root s=1.96 Tev
... At L1 the single electron triggers select events based on the energy deposited in the EM section of the calorimeter; typical L1 requirements are greater than 10 –15 GeV.. At L3, addi- ti[r] ... See full document
7
Measurements of the pp -gt; W gamma gamma and pp -gt; Z gamma gamma cross sections and limits on anomalous quartic gauge couplings at root s=8 TeV
... aQGC events are assigned a set of weights, each of which reproduces the effect of an anomalous ...diboson and triboson predictions are normalized to the NLO cross section predictions ob- tained with ... See full document
37
Measurement of the WZ production cross section in pp collisions at root s=7 and 8 TeV and search for anomalous triple gauge couplings at root s=8 TeV
... reconstructed from PF objects using the anti-k T clustering algorithm [ 35 , 36 ] with a size parameter R of ...obtained from the ECAL measure- ment. The energy of electrons is determined from a ... See full document
30
Evidence of Wγγ Production in pp Collisions at s=8 TeV and Limits on Anomalous Quartic Gauge Couplings with the ATLAS Detector
... (EM) and hadronic calorimeters, and a muon spectrometer (MS) immersed in the magnetic field produced by a system of superconducting ...toroids. Events in this analysis are selected with triggers ... See full document
26
Measurement of the $W^+W^-$ Cross section in $pp$ Collisions at $\sqrt{s} = 7$ TeV and Limits on Anomalous $WW\gamma$ and $WWZ$ couplings
... leptons from W boson decays are expected to be isolated from any other activity in the ...originating at the primary vertex of the event, which is chosen as the vertex with the highest ∑ p 2 T of its ... See full document
33
Study of $WW\gamma$ and $WZ\gamma$ production in $pp$ collisions at $\sqrt{s} = 8$ TeV and search for anomalous quartic gauge couplings with the ATLAS experiment
... ] at the LHC is a multipurpose particle detector with a forward-backward symmetric cylindrical geometry and a near 4π coverage in solid ...angle. 1 It consists of an inner tracking detector ... See full document
44
Search for WW gamma and WZ gamma production and constraints on anomalous quartic gauge couplings in pp collisions at root s=8 TeV
... based on the displaced vertex expected from b hadron ...efficiency, and has a 1% misidentification ...the WW γ and 10% of the WZ γ signal via the W → c¯s, Z → b¯b ... See full document
21
Search for $WW \gamma$ and $WZ \gamma$ production and constraints on anomalous quartic gauge couplings in $pp$ collisions at $\sqrt s =$ 8 TeV
... the limits on the WWγγ AQGC parameter obtained from this study, together with results from exclusive γγ → WW production at CMS [23] and results from the L3 [8] ... See full document
33
Search for anomalous couplings in boosted $\mathrm{ WW/WZ }\to\ell\nu\mathrm{ q \bar{q} }$ production in proton-proton collisions at $\sqrt{s} =$ 8 TeV
... 7 TeV analysis are replaced by analytical functions, which provide additional flexibility to model the data ...results from the first set of fits to perform an unbinned maximum-likelihood fit to data that ... See full document
22
Search for a Heavy Neutral Particle Decaying to $e\mu$, $e\tau$, or $\mu\tau$ in $pp$ Collisions at $\sqrt{s}=8$ TeV with the ATLAS Detector
... G.N. Hamity 146c , P.G. Hamnett 42 , L. Han 33b , K. Hanagaki 118 , K. Hanawa 156 , M. Hance 15 , P. Hanke 58a , R. Hanna 137 , J.B. Hansen 36 , J.D. Hansen 36 , M.C. Hansen 21 , P.H. Hansen 36 , K. Hara 161 , A.S. Hard ... See full document
25
Search for Higgs bosons decaying to $aa$ in the $\mu\mu\tau\tau$ final state in $pp$ collisions at $\sqrt{s} = $ 8 TeV with the ATLAS experiment
... arising from the electromagnetic and hadronic components of the show- ...lation and then improved and validated using ...pile-up from other pp interactions in the same or ... See full document
24
On the statistics of the product and the ratio of random envelopes taken from 'alfa'-'mu', 'eta'-'mu', e 'capa'-'mu' distributions : Estatísticas do produto e da razão de envoltórias de desvanecimento tomadas das distribuições 'alfa'-'mu', 'eta'-'mu', e 'capa'-'mu'
... η-µ, and κ-µ distributions are general fading models encompassing several tra- ditional fading models (Rayleigh, Nakagami-m, Hoyt, Rice and Weibull) as particular ...system and secrecy capacity are a ... See full document
151
Search for the flavour-changing neutral current B-s(0)->mu+mu- in p(p)over-bar collisions at root s=1.96 TeV with the D0 dectector
... C. E. Gerber, 48 Y. Gershtein, 71 G. Ginther, 66 T. Golling, 21 B. Go´mez, 70 K. Gounder, 47 A. Goussiou, 52 P. D. Grannis, 67 S. Greder, 18 H. Greenlee, 47 Z. D. Greenwood, 56 E. M. Gregores, 4 Ph. Gris, 12 J.-F. ... See full document
7
Search for $B^0_s \to \mu^+ \mu^-$ and $B^0 \to \mu^+ \mu^-$ decays
... signal and normalization samples is used in this ...the events that pass or fail the muon identification ...data and MC event ...muon and either a silicon track or a signal in the muon cham- ... See full document
35
Angular analysis of the decay B$^+$$\to$ K$^+\mu^+\mu^-$ in proton-proton collisions at $\sqrt{s} =$ 8 TeV
... RAS and RFBR (Russia); MESTD (Serbia); SEIDI, CPAN, PCTI and FEDER (Spain); Swiss Funding Agencies (Switzerland); MST (Taipei); ThEPCenter, IPST, STAR, and NSTDA (Thailand); TUBITAK and TAEK ... See full document
20
Aproximações para somas de envoltórias alpha-mu, eta-mu e kappa-mu via casamento de assíntotas = Approximations for sums of alpha-mu envelopes, eta-mu and kappa-mu via wedding asymptotes
... entre 1/2 e +∞, estando associado ao n´ umero de clusters de ...= 1, a distribui¸c˜ ao Nakagami-m coincide com a distribui¸c˜ ao ...= 1/2, corresponde a uma distribui¸c˜ ao Gaussiana ...< ... See full document
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