Search results for "electroweak interaction"

showing 10 items of 358 documents

The electroweak sector of the NMSSM at the one-loop level

2010

We present the electroweak spectrum for the Next-to-Minimal Supersymmetric Standard Model at the one-loop level, e. g. the masses of Higgs bosons, sleptons, charginos and neutralinos. For the numerical evaluation we present a mSUGRA variant with non-universal Higgs mass parameters squared and we compare our results with existing ones in the literature. Moreover, we briefly discuss the implications of our results for the calculation of the relic density.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsElectroweak interactionSpectrum (functional analysis)High Energy Physics::PhenomenologyFOS: Physical sciences01 natural sciencesLoop (topology)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHiggs bosonddc:530High Energy Physics::Experiment010306 general physicsParticle Physics - PhenomenologyMinimal Supersymmetric Standard ModelBoson
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extended MSSM

2012

We investigate the perturbative regime of the Minimal Supersymmetric Con- formal Technicolor and show that it allows for a stable vacuum correctly breaking the electroweak symmetry. We nd that the particle spectrum is richer than the MSSM one since it features several new particles stemming out from the new N = 4 sector of the theory. The parameter space of the new theory is reduced imposing naturalness of the cou- plings and soft supersymmetry breaking masses, perturbativity of the model at the EW scale as well as phenomenological constraints. By studying the RGEs at two loops we nd that the Yukawa couplings of the heavy fermionic states

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyElectroweak interactionYukawa potentialConformal mapTechnicolorParameter space01 natural sciencesSupersymmetry breakingSymmetry (physics)Naturalness0103 physical sciences010306 general physicsNuclear Physics B
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The simplest scoto-seesaw model: WIMP dark matter phenomenology and Higgs vacuum stability

2021

We analyze the consistency of electroweak breaking, neutrino and dark matter phenomenology within the simplest scoto-seesaw model. By adding the minimal dark sector to the simplest "missing partner" type-I seesaw one has a physical picture for the neutrino oscillation lengths: the "atmospheric" mass scale arises from the tree-level seesaw, while the "solar" scale is induced radiatively, mediated by the dark sector. We identify parameter regions consistent with theoretical constraints, as well as dark matter relic abundance and direct detection searches. Using two-loop renormalization group equations we explore the stability of the vacuum and the consistency of the underlying dark parity sym…

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsPhysicsQC1-999Dark matterElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesAstrophysics::Cosmology and Extragalactic Astrophysics01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometryDouble beta decay0103 physical sciencesHiggs bosonNeutrino010306 general physicsNeutrino oscillationPhenomenology (particle physics)Physics Letters B
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Scotogenic dark matter stability from gauged matter parity

2019

We explore the idea that dark matter stability results from the presence of a matter-parity symmetry, arising naturally as a consequence of the spontaneous breaking of an extended $\mathrm{SU(3) \otimes SU(3)_L \otimes U(1)_X \otimes U(1)_{N}}$ electroweak gauge symmetry with fully gauged B-L. Using this framework we construct a theory for scotogenic dark matter and analyze its main features.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsSpontaneous symmetry breakingDark matterElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesParity (physics)Stability result01 natural scienceslcsh:QC1-999High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicslcsh:PhysicsGauge symmetryPhysics Letters
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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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Precision measurement of the hadronic cross-section through the radiative return method

2002

Electron--positron annihilation into hadrons plus an energetic photon from initial-state radiation allows the hadronic cross-section to be measured over a wide range of energies at high luminosity meson factories. Weighted integrals over this cross-section are a decisive input for electroweak precision tests. A Monte Carlo event generator called PHOKHARA has been developed, which simulates $e^+ e^- \to$ hadrons + photon(s) at the NLO accuracy. The latest tests and upgrades are presented in this paper.

PhysicsNuclear and High Energy PhysicsParticle physicsAnnihilationLuminosity (scattering theory)PhotonMesonElectroweak interactionMonte Carlo methodHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaAtomic and Molecular Physics and OpticsHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Radiative transferHigh Energy Physics::ExperimentNuclear ExperimentParticle Physics - PhenomenologyEvent generator
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Implications of an axino LSP for naturalness

2014

Both the naturalness of the electroweak symmetry breaking and the resolution of the strong CP problem may require a small Higgsino mass $\mu$ generated by a realization of the DFSZ axion model. Assuming the axino is the lightest supersymmetric particle, we study its implications on $\mu$ and the axion scale. Copiously produced light Higgsinos at collider (effectively only neutral NLSP pairs) eventually decay to axinos leaving prompt multi-leptons or displaced vertices which are being looked for at the LHC. We use latest LHC7+8 results to derive current limits on $\mu$ and the axion scale. Various Higgsino-axino phenomenology is illustrated by comparing with a standard case without lightest …

PhysicsNuclear and High Energy PhysicsParticle physicsAxinoPhysics beyond the Standard ModelElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaLightest Supersymmetric ParticleHigh Energy Physics - PhenomenologyHigh Energy Physics::TheoryHigh Energy Physics - Phenomenology (hep-ph)Strong CP problemHigh Energy Physics::ExperimentHiggsinoPhenomenology (particle physics)Axion
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CKM matrix and fermion masses in the dualized standard model

1997

A Dualized Standard Model recently proposed affords a natural explanation for the existence of Higgs fields and of exactly 3 generations of fermions, while giving at the same time the observed fermion mass hierarchy together with a tree-level CKM matrix equal to the identity matrix. It further suggests a method for generating from loop corrections the lower generation masses and nondiagonal CKM matrix elements. In this paper, the proposed calculation is carried out to 1-loop. It is found first that with the method suggested one can account readily for the masses of the second generation fermions as a `leakage' from the highest generation. Then, with the Yukawa couplings fixed by fitting the…

PhysicsNuclear and High Energy PhysicsParticle physicsCabibbo–Kobayashi–Maskawa matrixElectroweak interactionHigh Energy Physics::PhenomenologyIdentity matrixYukawa potentialFOS: Physical sciencesFísicaFermionHigh Energy Physics - PhenomenologyStandard Model (mathematical formulation)High Energy Physics - Phenomenology (hep-ph)Higgs bosonFree parameter
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The tau weak-magnetic dipole moment

1994

We calculate the prediction for the anomalous weak-magnetic form factor of the tau lepton at $q^2=M_Z^2$ within the Standard Model. With all particles on-shell, this is a electroweak gauge invariant quantity. Its value is $a_\tau^w (M_Z^2)= - \;(2.10 + 0.61\, i) \times 10^{-6}$. We show that the transverse and normal components of the single-tau polarization of tau pairs produced at $e^+e^-$ unpolarized collisions are sensitive to the real and absorptive parts of the anomalous weak-magnetic dipole moment of the tau. The sensitivity one can achieve at LEP in the measurement of this dipole moment is discussed.

PhysicsNuclear and High Energy PhysicsParticle physicsCamps magnèticsMagnetic momentElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesInvariant (physics)Polarization (waves)Partícules (Física nuclear)Transverse planeDipoleHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentCamps Teoria quàntica deLeptonParticle Physics - Phenomenology
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Lepton-number violation and right-handed neutrinos in Higgs-less effective theories

2005

Following previous work, we identify a symmetry S_nat that generalizes the concept of custodial symmetry, keeping under control deviations from the Standard Model (SM). To realize S_nat linearly, the space of gauge fields has to be extended. Covariant constraints formulated in terms of spurions reduce S_nat back to SU(2)_L x U(1)_Y. This allows for a covariant introduction of explicit S_nat-breaking parameters. We assume that S_nat is at play in a theory of electroweak symmetry-breaking without a light Higgs particle. We describe some consequences of this assumption, using a non-decoupling effective theory in which the loop expansion procedure is based on both momentum and spurion power cou…

PhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theory010308 nuclear & particles physicsElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciences01 natural sciencesLepton numberCustodial symmetryStandard ModelHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]0103 physical sciencesEffective field theoryHiggs bosonSymmetry breaking010306 general physics
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