Search results for "SCALE"

showing 10 items of 5180 documents

Concluding talk at NOW 2006

2006

This writeup summarizes the status of neutrino oscillations, including recent fluxes and experimental data, as of summer 2006. A discussion is given on the current status of absolute scale of neutrino mass from tritium, neutrinoless double beta decay and cosmological observations, as well as the prospects for the next generation of experiments, including lepton flavor violation searches, and their theoretical significance.

PhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaAtomic and Molecular Physics and OpticsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Double beta decayHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationAbsolute scaleLepton
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Status after the first LHC run: Looking for new directions in the physics landscape

2015

The LHC data have confirmed the Standard Model as the correct theory at the electroweak scale. It successfully explains the experimental results with high precision and all its ingredients, including the Higgs boson, have been finally verified. At the same time, the negative searches for signals of new phenomena challenge our previous theoretical wisdom on new-physics scenarios.

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron Collider010308 nuclear & particles physicsPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyElectroweak interactionFOS: Physical sciencesTechnicolor01 natural sciencesHigh Energy Physics - ExperimentStandard ModelHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHiggs bosonGenerationElectroweak scale010306 general physicsInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Modelling tribimaximal neutrino mixing

2009

We model tribimaximal lepton mixing from first principles in a way that avoids the problem of the vacuum alignment characteristic of such models. This is achieved by using a softly broken A(4) symmetry realized with an isotriplet fermion, also triplet under A(4). No scalar A(4) triplet is introduced. This represents one possible realization of general schemes characterized by the minimal set of either three or five physical parameters. In the three parameter versions the neutrinoless double beta mass parameter m(ee) vanishes, while in the five parameter schemes the absolute scale of neutrino mass, although not predicted, is related to the two Majorana phases. The model realization we discus…

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderHigh Energy Physics::PhenomenologyScalar (mathematics)FísicaFOS: Physical sciencesFermionMAJORANAHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)NeutrinoMass parameterAbsolute scaleLepton
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Bosonic quartic couplings at CERN LHC

2004

We analyze the potential of the CERN Large Hadron Collider (LHC) to study anomalous quartic vector-boson interactions Z Z gamma gamma, Z Z Z gamma, W+ W- gamma gamma, and W+ W- Z gamma through the weak boson fusion processes q q -> q q gamma gamma and q q -> q q gamma Z(-> l+ l-) with l = electron or muon. After a careful study of the backgrounds and how to extract them from the data, we show that the process p p -> j j gamma l+ l- is potentially the most sensitive to deviations from the Standard Model, improving the sensitivity to anomalous couplings by up to a factor 10^4 (10^2) with respect to the present direct (indirect) limits.

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderScale (ratio)010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaAcceleradors de partículesHigh Energy Physics::PhenomenologyStructure (category theory)7. Clean energy01 natural sciencesPartícules (Física nuclear)Particle acceleratorsStandard ModelPhoton emissionQuartic function0103 physical sciencesFermilab010306 general physicsBosonsParticles (Nuclear physics)Gauge symmetryPhysical Review D
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Supersymmetric mass spectra and the seesaw scale

2011

Supersymmetric mass spectra within two variants of the seesaw mechanism, commonly known as type-II and type-III seesaw, are calculated using full 2-loop RGEs and minimal Supergravity boundary conditions. The type-II seesaw is realized using one pair of 15 and $\bar{15}$ superfields, while the type-III is realized using three copies of $24_M$ superfields. Using published, estimated errors on SUSY mass observables attainable at the LHC and in a combined LHC+ILC analysis, we calculate expected errors for the parameters of the models, most notably the seesaw scale. If SUSY particles are within the reach of the ILC, pure mSugra can be distinguished from mSugra plus type-II or type-III seesaw for…

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderScale (ratio)010308 nuclear & particles physicsSupergravityFOS: Physical sciencesFísicaObservableSupersymmetryParameter space01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw mechanismSeesaw molecular geometry0103 physical sciences010306 general physics
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Supersymmetric Extension of Technicolor & Fermion Mass Generation

2012

We provide a complete extension of Minimal Walking Technicolor able to account for the standard model fermion masses. The model is supersymmetric at energies greater or equal to the technicolor compositeness scale. We integrate out, at the supersymmetry breaking scale, the elementary Higgses. We use the resulting four-fermion operators to derive the low energy effective theory. We then determine the associated tree-level vacuum and low energy spectrum properties. Furthermore we investigate the phenomenological viability of the model by comparing its predictions with electroweak precision tests and experimental bounds on the mass spectrum. We then turn to the composite Higgs phenomenology at…

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderSupersymmetry breaking scaleta114010308 nuclear & particles physicsElectroweak interactionMass generationHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyFOS: Physical scienceshep-latTechnicolorhep-ph7. Clean energy01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesEffective field theoryHiggs boson010306 general physicsMinimal Supersymmetric Standard Model
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Non-decoupling of Heavy Neutrinos and Lepton Flavour Violation

1995

We consider a class of models predicting new heavy neutral fermionic states, whose mixing with the light neutrinos can be naturally significant and produce observable effects below the threshold for their production. We update the indirect limits on the flavour non-diagonal mixing parameters that can be derived from unitarity, and show that significant rates are in general expected for one-loop-induced rare processes due to the exchange of virtual heavy neutrinos, involving the violation of the muon and electron lepton numbers. In particular, the amplitudes for $\mu$--$e$ conversion in nuclei and for $\mu\to ee^+e^-$ show a non-decoupling quadratic dependence on the heavy neutrino mass $M$,…

PhysicsNuclear and High Energy PhysicsParticle physicsMuonUnitarityHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesObservableDecoupling (cosmology)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentNeutrinoElectroweak scaleMixing (physics)Particle Physics - PhenomenologyLepton
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CPT Violation and the Nature of Neutrinos

2002

In order to accommodate the neutrino oscillation signals from the solar, atmospheric, and LSND data, a sterile fourth neutrino is generally invoked, though the fits to the data are becoming more and more constrained. However, it has recently been shown that the data can be explained with only three neutrinos, if one invokes CPT violation to allow different masses and mixing angles for neutrinos and antineutrinos. We explore the nature of neutrinos in such CPT-violating scenarios. Majorana neutrino masses are allowed, but in general, there are no longer Majorana neutrinos in the conventional sense. However, CPT-violating models still have interesting consequences for neutrinoless double beta…

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryPhysics::Instrumentation and DetectorsHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesNuclear Theory (nucl-th)MAJORANAHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Double beta decayMass scaleHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationMixing (physics)
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Single-photon Z decays and small neutrino masses

1996

We discuss some rare Z decay signatures associated with extensions of the Standard Model with spontaneous lepton number violation at the electroweak scale. We show that single-photon Z decays such as $Z \to \gamma H$ and $Z \to \gamma J J$ where H is a CP-even Higgs boson and J denotes the associated CP-odd Majoron may occur with branching ratios accessible to LEP sensitivities, even though the corresponding neutrino masses can be very small, as required in order to explain the deficit of solar neutrinos.

PhysicsNuclear and High Energy PhysicsParticle physicsPhotonSolar neutrinoHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaLepton numberHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Higgs bosonHigh Energy Physics::ExperimentNeutrinoElectroweak scaleMajoron
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KATRIN, a next generation tritium β decay experiment in search for the absolute neutrino mass scale

2002

Abstract With the compelling evidence for massive neutrinos from recent ν-oscillation experiments, one of the most fundamental tasks of particle physics over the next years will be the determination of the absolute mass scale of neutrinos, which has crucial implications for cosmology, astrophysics and particle physics. A next generation tritium β decay experiment, the Karlsruhe Tritium Neutrino experiment (KATRIN), is proposed to reach a sub eV sensitivity on the absolute mass of the electron neutrino.

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsSolar neutrinoSolar neutrino problemCosmologyNuclear physicsHigh Energy Physics::ExperimentTritiumMass scaleNeutrinoElectron neutrinoKATRINProgress in Particle and Nuclear Physics
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