Search results for "The Standard Model"

showing 10 items of 466 documents

Nonstandard Yukawa couplings and Higgs portal dark matter

2015

We study the implications of non-standard Higgs Yukawa couplings to light quarks on Higgs-portal dark matter phenomenology. Saturating the present experimental bounds on up-quark, down-quark, or strange-quark Yukawa couplings, the predicted direct dark matter detection scattering rate can increase by up to four orders of magnitude. The effect on the dark matter annihilation cross section, on the other hand, is subleading unless the dark matter is very light -- a scenario that is already excluded by measurements of the Higgs invisible decay width. We investigate the expected size of corrections in multi-Higgs-doublet models with natural flavor conservation, the type-II two-Higgs-doublet mode…

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsAnnihilation010308 nuclear & particles physicsHigh Energy Physics::LatticePhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyDark matterYukawa potentialFOS: Physical sciences01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Composite Higgs models0103 physical sciencesHiggs bosonHigh Energy Physics::Experiment010306 general physicsPhenomenology (particle physics)Journal of High Energy Physics
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New physics effects in tree-level decays and the precision in the determination of the quark mixing angle γ.

2015

We critically review the assumption that no new physics is acting in tree-level B-meson decays and study the consequences for the ultimate precision in the direct determination of the Cabibbo-Kobayashi-Maskawa (CKM) angle γ. In our exploratory study we find that sizeable universal new physics contributions, ΔC1,2, to the tree-level Wilson coefficients C1,2 of the effective Hamiltonian describing weak decays of the b quark are currently not excluded by experimental data. In particular, we find that ImΔC1 and ImΔC2 can easily be of order ±10% without violating any constraints from data. Such a size of new physics effects in C1 and C2 corresponds to an intrinsic uncertainty in the CKM angle γ …

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsCabibbo–Kobayashi–Maskawa matrixPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyObservableBottom quarksymbols.namesakesymbolsHeavy quark effective theoryHigh Energy Physics::ExperimentHamiltonian (quantum mechanics)
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Charge asymmetries of top quarks at hadron colliders revisited

2011

A sizeable difference in the differential production cross section of top- compared to antitop-quark production, denoted charge asymmetry, has been observed at the Tevatron. The experimental results seem to exceed the theory predictions based on the Standard Model by a significant amount and have triggered a large number of suggestions for "new physics". In the present paper the Standard Model predictions for Tevatron and LHC experiments are revisited. This includes a reanalysis of electromagnetic as well as weak corrections, leading to a shift of the asymmetry by roughly a factor 1.1 when compared to the results of the first papers on this subject. The impact of cuts on the transverse mome…

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron Collider010308 nuclear & particles physicsmedia_common.quotation_subjectPhysics beyond the Standard ModelHadronTevatronFísicaFOS: Physical sciences01 natural sciencesAsymmetryHigh Energy Physics - ExperimentStandard ModelHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesRapidityHigh Energy Physics::Experiment010306 general physicsmedia_common
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Dijets at Tevatron Cannot Constrain SMEFT Four-Quark Operators

2019

We explore the sensitivity of Tevatron data to heavy new physics effects in differential dijet production rates using the SMEFT in light of the fact that consistent and conservative constraints from the LHC cannot cover relatively low cutoff scales in the EFT. In contrast to the results quoted by the experimental collaborations and other groups, we find that, once consistency of the perturbation expansion is enforced and reasonable estimates of theoretical errors induced by the SMEFT series in $\frac{E}{\Lambda}$ are included, there is no potential to constrain four-quark contact interactions using Tevatron data. This shows the general difficulty of constraining physics model-independently …

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderLuminosity (scattering theory)Physics beyond the Standard ModelHigh Energy Physics::PhenomenologyTevatronFOS: Physical sciencesEffective Field TheoriesLambdaComputer Science::Digital LibrariesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Beyond Standard ModelComputer Science::Mathematical SoftwareCutofflcsh:QC770-798lcsh:Nuclear and particle physics. Atomic energy. RadioactivityHigh Energy Physics::ExperimentSensitivity (control systems)
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LHC-scale left-right symmetry and unification

2013

We construct a comprehensive list of nonsupersymmetric standard model extensions with a low-scale left-right (LR)-symmetric intermediate stage that may be obtained as simple low-energy effective theories within a class of renormalizable SO(10) grand unified theories. Unlike the traditional minimal LR models many of our example settings support a perfect gauge coupling unification even if the LR scale is in the LHC domain at a price of only (a few copies of) one or two types of extra fields pulled down to the TeV-scale ballpark. We discuss the main aspects of a potentially realistic model building conforming the basic constraints from the quark and lepton sector flavor structure, proton deca…

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderScale (ratio)Proton decayPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaHigh Energy Physics - PhenomenologyStandard Model (mathematical formulation)High Energy Physics - Phenomenology (hep-ph)Grand Unified TheoryModel buildingPhysical Review D
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The Weak-Magnetic Moment of Heavy Quarks

1997

With initial and final particles on-shell, the anomalous weak-magnetic dipole moments of b and c quarks are electroweak gauge invariant quantities of the effective couplings Zb\bar{b} and Zc\bar{c}, respectively, and good candidates to test the Standard Model and/or new physics. Here we present a complete computation of these quantities within the Standard Model. We show that decoupling properties with respect to heavy particles do take place in the weak magnetic moment. The obtained values, a_b(M_Z^2)=(2.98-1.56i)x10^(-4) and a_c(M_Z^2)=(-2.80+1.09i)x10^(-5) are dominated by one-gluon exchange diagrams. The electroweak corrections are less than 1% of the total magnitude.

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsMagnetic momentPhysics beyond the Standard ModelComputationElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesDecoupling (cosmology)Invariant (physics)Partícules (Física nuclear)DipoleHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::Experiment
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Semileptonic decays of light quarks beyond the Standard Model

2009

We describe non-standard contributions to semileptonic processes in a model independent way in terms of in SU(2)(L) x U(1)(Y) invariant effective lagrangian at the weak scale, front which we derive the low-energy effective lagrangian governing muon and beta decays. We find that the deviation from Cabibbo universality, Delta(CKM) equivalent to vertical bar V-ud vertical bar(2) + vertical bar V-us vertical bar(2) + vertical bar V-ub vertical bar(2) - 1, receives contributions from four effective operators. The phenomenological bound Delta(CKM) = (-1 +/- 6) x 10(-4) provides strong constraints on all four operators, corresponding to art effective scale Lambda > 11 TeV (90% CL). Depending on th…

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsMuonCabibbo–Kobayashi–Maskawa matrixPhysics beyond the Standard ModelElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesObservableHigh Energy Physics - PhenomenologyOperator (computer programming)High Energy Physics - Phenomenology (hep-ph)Effective field theoryHigh Energy Physics::Experiment
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Heavy quarks and tau leptons: New physics opportunities

2014

In this talk I discuss the role of heavy quarks in new physics searches with tau leptons. I focus on new physics effects associated to the scalar sector which are naturally enhanced for the heaviest fermions due to the large hierarchy of the fermion masses. I will discuss two topics within this context: lepton flavour violation in the $\tau - \ell$ ($\ell=e,\mu$) sector and violations of lepton universality in tauonic $B$ decays.

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsPhysics beyond the Standard ModelHigh Energy Physics::LatticeFlavourHigh Energy Physics::PhenomenologyFOS: Physical sciencesFermionUniversality (dynamical systems)High Energy Physics - ExperimentHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentLepton
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D–D¯ mixing and new physics: General considerations and constraints on the MSSM

2007

Abstract Combining the recent experimental evidence of D – D ¯ mixing, we extract model-independent information on the mixing amplitude and on its CP-violating phase. Using this information, we present new constraints on the flavour structure of up-type squark mass matrices in supersymmetric extensions of the Standard Model.

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologySuperpartnerCP violationHigh Energy Physics::ExperimentSupersymmetryMass matrixMixing (physics)Standard ModelPhysics Letters B
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High scale mixing relations as a natural explanation for large neutrino mixing

2015

The origin of small mixing among the quarks and a large mixing among the neutrinos has been an open question in particle physics. In order to answer this question, we postulate general relations among the quarks and the leptonic mixing angles at a high scale, which could be the scale of Grand Unified Theories. The central idea of these relations is that the quark and the leptonic mixing angles can be unified at some high scale either due to some quark-lepton symmetry or some other underlying mechanism and as a consequence, the mixing angles of the leptonic sector are proportional to that of the quark sector. We investigate the phenomenology of the possible relations where the leptonic mixin…

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsUnification010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::LatticePhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyFOS: Physical sciencesAstronomy and AstrophysicsNew Physics ; GUT ; CKM Matrix01 natural sciencesAtomic and Molecular Physics and OpticsHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesGrand Unified TheoryHigh Energy Physics::ExperimentNeutrino010306 general physicsPhenomenology (particle physics)International Journal of Modern Physics A
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