Search results for "Technicolor"

showing 10 items of 62 documents

Consistent searches for SMEFT effects in non-resonant dijet events

2018

We investigate the bounds which can be placed on generic new-physics contributions to dijet production at the LHC using the framework of the Standard Model Effective Field Theory, deriving the first consistently-treated EFT bounds from non-resonant high-energy data. We recast an analysis searching for quark compositeness, equivalent to treating the SM with one higher-dimensional operator as a complete UV model. In order to reach consistent, model-independent EFT conclusions, it is necessary to truncate the EFT effects consistently at order $1/\Lambda^2$ and to include the possibility of multiple operators simultaneously contributing to the observables, neither of which has been done in prev…

Nuclear and High Energy PhysicsParticle physicsTevatronFOS: Physical sciencesParameter space01 natural sciencesHigh Energy Physics - ExperimentStandard ModelHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Perturbative QCD0103 physical sciencesEffective field theorylcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsLinear combinationPhysicsLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyEffective Field TheoriesTechnicolor and Composite ModelsObservableWeinberg angleHigh Energy Physics - PhenomenologyBeyond Standard Modellcsh:QC770-798Journal of High Energy Physics
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The physics programme of the MoEDAL experiment at the LHC

2014

The MoEDAL experiment at Point 8 of the LHC ring is the seventh and newest LHC experiment. It is dedicated to the search for highly ionizing particle avatars of physics beyond the Standard Model, extending significantly the discovery horizon of the LHC. A MoEDAL discovery would have revolutionary implications for our fundamental understanding of the Microcosm. MoEDAL is an unconventional and largely passive LHC detector comprised of the largest array of Nuclear Track Detector stacks ever deployed at an accelerator, surrounding the intersection region at Point 8 on the LHC ring. Another novel feature is the use of paramagnetic trapping volumes to capture both electrically and magnetically ch…

Nuclear and High Energy PhysicsParticle physicsphysics beyond the Standard ModelAtomic and Molecular Physics and Opticdoubly charged particlePhysics::Instrumentation and DetectorsPhysics beyond the Standard Modelmagnetic monopoleFOS: Physical sciencesLHC magnetic monopoletechnicolor01 natural sciencesdark matterData acquisitionHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences(pseudo-)stable massive charged particle010306 general physicsNuclear and High Energy PhysicParticle Physics - PhenomenologyPhysicsLarge Hadron Collider010308 nuclear & particles physicsDetectorsupersymmetryFísicaAstronomy and AstrophysicsMoEDALAtomic and Molecular Physics and Opticsextra dimensionmonopoliumHigh Energy Physics - PhenomenologyMoEDAL experimentNuclear trackhighly ionizing particlesupersymmetrydyonINTERNATIONAL JOURNAL OF MODERN PHYSICS A
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The search for dark matter gauge bosons with the Mainz Microtron

2011

Abstract A pilot experiment in the search for light gauge bosons at the spectrometer setup of the A1 collaboration at MAMI is presented. Light gauge bosons arise naturally in a wide range of theoretical approaches beyond the standard model and are in accordance with several pieces of experimental evidence not yet understood in the standard model. A first test measurement at MAMI showed that existing limits on the coupling of such a light gauge boson can be improved by nearly an order of magnitude by fixed target experiments at existing electron accelerators.

Nuclear physicsHidden sectorPhysicsNuclear and High Energy PhysicsGauge bosonParticle physicsSpectrometerPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyDark matterTechnicolorMicrotronStandard ModelProgress in Particle and Nuclear Physics
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A model for dark matter, naturalness and a complete gauge unification

2015

We consider dark matter in a minimal extension of the Standard Model (SM) which breaks electroweak symmetry dynamically and leads to a complete unification of the SM and technicolor coupling constants. The unification scale is determined to be $M_{\rm U} \approx 2.2 \times 10^{15}$ GeV and the unified coupling $\alpha_{\rm U} \approx 0.0304$. Moreover, unification strongly suggest that the technicolor sector of the model must become strong at the scale of ${\cal O}$(TeV). The model also contains a tightly constrained sector of mixing neutral fields stabilized by a discrete symmetry. We find the lightest of these states can be DM with a mass in the range $m_{\rm DM} \approx 30-800$ GeV. We f…

Particle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Dark matterFOS: Physical sciencesTechnicolorParameter space01 natural sciences7. Clean energyStandard ModelHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsCoupling constantPhysicsdark matter theory010308 nuclear & particles physicsdark matter experimentsElectroweak interactionHigh Energy Physics::PhenomenologyAstronomy and AstrophysicsCoupling (probability)High Energy Physics - Phenomenologyparticle physics - cosmology connectionHigh Energy Physics::ExperimentDiscrete symmetryAstrophysics - Cosmology and Nongalactic AstrophysicsJournal of Cosmology and Astroparticle Physics
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Search for high-mass resonances decaying to dilepton final states in pp collisions at √s = 7 TeV with the ATLAS detector

2012

The ATLAS detector at the Large Hadron Collider is used to search for high-mass resonances decaying to an electron-positron pair or a muon-antimuon pair. The search is sensitive to heavy neutral Z′ gauge bosons, Randall-Sundrum gravitons, Z [superscript *] bosons, techni-mesons, Kaluza-Klein Z/γ bosons, and bosons predicted by Torsion models. Results are presented based on an analysis of pp collisions at a center-of-mass energy of 7 TeV corresponding to an integrated luminosity of 4.9 fb[superscript −1] in the e [superscript +] e [superscript −] channel and 5.0 fb[superscript −1] in the μ [superscript +] μ [superscript −] channel. A Z [superscript ′] boson with Standard Model-like couplings…

Particle physicsNuclear and High Energy PhysicsPhysics::General PhysicsCiências Naturais::Ciências Físicas:Ciências Físicas [Ciências Naturais]Kaluza–Klein theoryTechnicolorddc:500.27. Clean energy01 natural sciences530Nuclear physics0103 physical sciencesddc:530EXTRA DIMENSIONSHigh Energy Physics010306 general physicsCiencias Exactashadron-hadron scatteringBosonPhysicsddc:539Gauge bosonLarge Hadron ColliderHadron-Hadron scattering; Nuclear and High Energy PhysicsScience & TechnologyHadron-Hadron ScatteringATLAS detector010308 nuclear & particles physicsSettore FIS/01 - Fisica SperimentaleHigh Energy Physics::PhenomenologyGravitonFísicaATLASExtra dimensionsRandall–Sundrum modelHADRON-HADRON COLLISIONSExperimental High Energy PhysicsComputingMethodologies_DOCUMENTANDTEXTPROCESSINGFísica nuclearproton-proton collisionsHigh Energy Physics::ExperimentLHC
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Top-seesaw assisted technicolor model with 126 GeV Higgs boson

2013

We discuss a model which involves the top quark condensation and the walking technicolor. We focus on the scalar boson in such a model from the viewpoint of the observed scalar boson at the LHC.

PhysicsCondensed Matter::Quantum GasesTop quarkParticle physicsLarge Hadron ColliderHigh Energy Physics::PhenomenologyFOS: Physical sciencesTechnicolorScalar bosonHigh Energy Physics - PhenomenologyGeneral Relativity and Quantum CosmologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometryHiggs bosonHigh Energy Physics::ExperimentFocus (optics)
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Electroweak precision data and right-handed gauge bosons

1998

The implication of recent electroweak precision data for left-right symmetric models is examined. We establish a lower bound on the charged and neutral right-handed gauge bosons independent of the right-handed neutrino mass and of any restrictions or implied symmetries on the right KM matrix.

PhysicsGauge bosonParticle physicsPhysics and Astronomy (miscellaneous)Right handedCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::PhenomenologyElectroweak interactionTechnicolorUpper and lower boundsQuantum electrodynamicsHomogeneous spaceNeutrinoEngineering (miscellaneous)The European Physical Journal C
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Flavor constraints in a bosonic technicolor model

2011

Flavor constraints in a bosonic Technicolor model are considered. We illustrate different sources for their origin, and emphasize in particular the role played by the vector states present in the Technicolor model. This feature is the essential difference in comparison to an analogous model with two fundamental Higgs scalar doublets.

PhysicsHigh Energy Physics - PhenomenologyNuclear and High Energy PhysicsParticle physicsHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::PhenomenologyScalar (mathematics)Higgs bosonFOS: Physical sciencesHigh Energy Physics::ExperimentTechnicolorFlavorPhysical Review D
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Negative S parameter from holographic technicolor.

2006

We present a new class of 5D models, Holographic Technicolor, which fulfills the basic requirements for a candidate of comprehensible 4D strong dynamics at the electroweak scale. It is the first Technicolor-like model able to provide a vanishing or even negative tree-level S parameter, avoiding any no-go theorem on its sign. The model is described in the large-N regime. S is therefore computable: possible corrections coming from boundary terms follow the 1/N suppression, and generation of fermion masses and the S parameter issue do split up. We investigate the model's 4D dual, probably walking Technicolor-like with a large anomalous dimension.

PhysicsHigh Energy Physics::PhenomenologyGeneral Physics and AstronomyDuality (optimization)Boundary (topology)FOS: Physical sciencesTechnicolorFermionDual (category theory)Theoretical physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Dimension (vector space)Quantum mechanicsElectroweak scaleSign (mathematics)Physical review letters
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Neutrino electron scattering and electroweak gauge structure: Future tests

1997

Low-energy high-resolution neutrino-electron scattering experiments may play an important role in testing the gauge structure of the electroweak interaction. We propose the use of radioactive neutrino sources (e.g. $^{51}$Cr) in underground experiments such as BOREXINO, HELLAZ and LAMA. As an illustration, we display the sensitivity of these detectors in testing the possible existence of extra neutral gauge bosons, both in the framework of E_6 models and of models with left-right symmetry.

PhysicsNuclear and High Energy PhysicsGauge bosonParticle physicsNeutral currentPhysics::Instrumentation and DetectorsElectroweak interactionAstrophysics (astro-ph)High Energy Physics::PhenomenologyFOS: Physical sciencesFísicaTechnicolorAstrophysicsSymmetry (physics)Nuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentNeutrinoBorexinoCharged current
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