Search results for "Standard Model"

showing 10 items of 1206 documents

Jet substructure measurements of interference in non-interfering SMEFT effects

2019

The tails of diboson production at the LHC are sensitive to the interference between Standard Model and higher dimension operators parameterizing the effects of heavy new physics. However, helicity selection rules for the diboson scattering amplitudes set an obstruction to the na\"ive interference contributions of dimension six operators, causing the total diboson rate correction's leading contribution to cancel. In this case, carefully measuring the azimuthal decay angles "resurrects" the interference, recouping sensitivity to the "non-interfering" operators. We explore these signatures in detail, and find that the EFT uncertainties associated with higher-dimensional operators are uniquely…

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsmedia_common.quotation_subjectPhysics beyond the Standard ModelFOS: Physical sciencesObservableInterference (wave propagation)01 natural sciencesHelicityAsymmetryStandard ModelScattering amplitudeHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesJetslcsh:QC770-798lcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsmedia_commonBosonJournal of High Energy Physics
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Energy-independent new physics in the flavour ratios of high-energy astrophysical neutrinos

2010

We have studied the consequences of breaking the CPT symmetry in the neutrino sector, using the expected high-energy neutrino flux from distant cosmological sources such as active galaxies. For this purpose we have assumed three different hypotheses for the neutrino production model, characterised by the flavour fluxes at production phi(0)(e) : phi(0)(mu) : phi(0)(tau) = 1 : 2 : 0, 0 : 1 : 0, and 1 : 0 : 0, and studied the theoretical and experimental expectations for the muon-neutrino flux at Earth, phi(mu), and for the flavour ratios at Earth, R = phi(mu)/phi(e) and S = phi(tau)/phi(mu). CPT violation (CPTV) has been implemented by adding an energy-independent term to the standard neutrin…

PhysicsNuclear and High Energy PhysicsParticle physicsActive galactic nucleusCPT symmetryPhysics beyond the Standard ModelFísicaFOS: Physical sciencesSeparable spacesymbols.namesakeHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Astrophysical neutrinossymbolsLarge deviations theoryCPT violationNeutrinoHamiltonian (quantum mechanics)Neutrino oscillation
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Gravitational violation of R parity and its cosmological signatures

1996

The discrete R-parity ($R_P$) usually imposed on the Supersymmetric (SUSY) models is expected to be broken at least gravitationally. If the neutralino is a dark matter particle its decay channels into positrons, antiprotons and neutrinos are severely constrained from astrophysical observations. These constraints are shown to be violated even for Planck-mass-suppressed dimension-five interactions arising from gravitational effects. We perform a general analysis of gravitationally induced $R_P$ violation and identify two plausible and astrophysically consistent scenarios for achieving the required suppression.

PhysicsNuclear and High Energy PhysicsParticle physicsAge of the universeDark matterHigh Energy Physics::PhenomenologyPlanck massFOS: Physical sciencesFísicaSupersymmetryLightest Supersymmetric ParticleHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)R-parityNeutralinoHigh Energy Physics::ExperimentMinimal Supersymmetric Standard Model
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Search for the Standard Model Higgs boson in e+e− collisions at =161, 170 172

1997

The reaction e(+)e(-) --> HZ is used to search for the Standard Model Higgs boson, The data sample consists of integrated luminosities of 10.9 pb(-1), 1.1 pb(-1), and 9.5 pb(-1) collected by the ALEPH experiment at LEP during 1996, at centre-of-mass energies of 161, 170 and 172 GeV, respectively. No candidate events were found, in agreement with the expected background of 0.84 events from all Standard Model processes. This search results in a 95% C.L. lower limit on the Higgs boson mass of 69.4 GeV/c(2). When combined with earlier ALEPH searches performed at energies at and around the Z peak, this limit increases to 70.7 GeV/c(2). (C) 1997 Elsevier Science B.V.

PhysicsNuclear and High Energy PhysicsParticle physicsAleph010308 nuclear & particles physics01 natural sciencesLower limitStandard ModelNuclear physics0103 physical sciencesHiggs bosonLimit (mathematics)010306 general physicsALEPH experimentPhysics Letters B
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Observation of an excess in the search for the Standard Model Higgs boson at ALEPH

2000

A search has been performed for the Standard Model Higgs boson in the data sample collected with the ALEPH detector at LEP, at centre-of-mass energies up to 209GeV. An excess of 3sigma beyond the background expectation is found, consistent with the production of the Higgs boson with a mass near 114GeV/c2. Much of this excess is seen in the four-jet analyses, where three high purity events are selected.

PhysicsNuclear and High Energy PhysicsParticle physicsAlephResearch Groups and Centres\Physics\Low Temperature Physics010308 nuclear & particles physicsENERGIESFaculty of Science\PhysicsElectron–positron annihilationDetectorHigh Energy Physics::PhenomenologyFOS: Physical sciences01 natural sciencesHigh Energy Physics - ExperimentStandard ModelNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciencesHiggs boson[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]High Energy Physics::Experiment010306 general physicsParticle Physics - Experiment
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CPasymmetries inBsdecays and spontaneousCPviolation

1999

We study the possible effects of new physics in $\mathrm{CP}$ asymmetries in two-body ${B}_{s}$ decays in left-right models with spontaneous $\mathrm{CP}$ violation. Considering the contributions of new $\mathrm{CP}$ phases to the ${B}_{s}$ mixing as well as to the penguin-dominated decay amplitudes we show that, with the present constraints, large deviations from the standard model predictions in $\mathrm{CP}$ asymmetries are allowed in both cases. The detection of new physics can be achieved by measuring nonzero asymmetries which are predicted to vanish in the standard model or by comparing two measurements which are predicted to be equal in the standard model. In particular, we show that…

PhysicsNuclear and High Energy PhysicsParticle physicsAmplitudePhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyElectroweak interactionCP violationHigh Energy Physics::ExperimentLarge deviations theoryMixing (physics)Standard ModelPhysical Review D
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General flavor blind minimal supersymmetric standard model andCPviolation

2001

We study the implications on flavor changing neutral current and $\mathrm{CP}$ violating processes in the context of supersymmetric theories without a new flavor structure (flavor blind supersymmetry). The low-energy parameters are determined by the running of the soft breaking terms from the grand unified scale with supersymmetric (SUSY) phases consistent with the electric dipole moment constraints. We find that the $\mathrm{CP}$ asymmetry in $\stackrel{\ensuremath{\rightarrow}}{b}s\ensuremath{\gamma}$ can reach large values potentially measurable at B factories, especially in the low $BR(\stackrel{\ensuremath{\rightarrow}}{b}s\ensuremath{\gamma})$ region, while the contributions to electr…

PhysicsNuclear and High Energy PhysicsParticle physicsAnomalous magnetic dipole moment010308 nuclear & particles physicsFlavor-changing neutral currentHigh Energy Physics::PhenomenologySupersymmetry01 natural sciencesElectric dipole momentChargino0103 physical sciencesGrand Unified TheoryCP violationHigh Energy Physics::Experiment010306 general physicsMinimal Supersymmetric Standard ModelPhysical Review D
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Hadronic contribution to the lepton anomalous magnetic moment and pion form factor in lattice QCD

2012

Abstract The Mainz lattice QCD group is currently carrying out simulations of lattice QCD with the aim of making predictions for a wide range of phenomenologically relevant Standard Model properties. Here we present progress in understanding and controlling systematic effects in the computation of the pion vector form factor and the leading hadronic contribution to the lepton anomalous magnetic moment.

PhysicsNuclear and High Energy PhysicsParticle physicsAnomalous magnetic dipole moment010308 nuclear & particles physicsHigh Energy Physics::LatticeComputationNuclear TheoryHigh Energy Physics::PhenomenologyHadronForm factor (quantum field theory)Lattice QCD01 natural sciencesNuclear physicsStandard Model (mathematical formulation)Pion0103 physical sciencesHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsLeptonProgress in Particle and Nuclear Physics
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Tau spin correlations and the anomalous magnetic moment

2009

We show that the precise determination of the Tau magnetic properties is possible in the next generation accelerators, specially at B/Flavour factories. We define spin correlation observables suitable to extract the real part of the magnetic form factor that, for the first time, will allow to test the standard model-QED predictions. In particular, the predicted QED-dependence with both the momentum transfer and the lepton mass can be precisely measured. Until now, the most stringent bounds on the $\tau$ magnetic moment $a_\tau$ come from LEP data with strong assumptions on the physics involved on the observed process. In this paper, we find three different combinations of spin correlations …

PhysicsNuclear and High Energy PhysicsParticle physicsAnomalous magnetic dipole momentMagnetic momentAcceleradors de partículesMomentum transferElectromagnetic processes and propertiesFOS: Physical sciencesObservableElectronPartícules (Física nuclear)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)AmplitudeMagnetic form factorHigh Energy Physics::ExperimentLeptonStandard model
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Big-bang nucleosynthesis and the relic abundance of dark matter in a stau-neutralino coannihilation scenario

2008

A scenario of the Big-Bang Nucleosynthesis is analyzed within the Minimal Supersymmetric Standard Model which is consistent with a stau-neutralino coannihilation scenario to explain the relic abundance of dark matter. We find that we can account for the possible descrepancy of the abundance of $\mathrm{^{7}Li}$ between the observation and the prediction of the Big-Bang Nucleosynthesis by taking the mass of the neutralino as $300 \mathrm{GeV}$ and the mass difference between the stau and the neutralino as $(100 -- 120) MeV$. We can therefore simultaneously explain the abundance of the dark matter and that of $\mathrm{^{7}Li}$ by these values of parameters. The lifetime of staus in this scena…

PhysicsNuclear and High Energy PhysicsParticle physicsAstrophysics (astro-ph)High Energy Physics::PhenomenologyDark matterFOS: Physical sciencesSupersymmetryAstrophysicsStandard ModelHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Big Bang nucleosynthesisNucleosynthesisNeutralinoAstrophysics::Solar and Stellar AstrophysicsHigh Energy Physics::ExperimentLight dark matterAstrophysics::Galaxy AstrophysicsMinimal Supersymmetric Standard ModelPhysical Review D
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