Search results for "Electroweak scale"

showing 10 items of 31 documents

WCxf: An exchange format for Wilson coefficients beyond the Standard Model

2018

We define a data exchange format for numerical values of Wilson coefficients of local operators parameterising low-energy effects of physics beyond the Standard Model. The format facilitates interfacing model-specific Wilson coefficient calculators, renormalisation group (RG) runners, and observable calculators. It is designed to be unambiguous (defining a non-redundant set of operators with fixed normalisation in each basis), extensible (allowing the addition of new EFTs or bases by the user), and robust (being based on industry standard file formats with parsers implemented in many programming languages). We have implemented the format for the Standard Model EFT (SMEFT) and for the weak e…

EFTSParsing010308 nuclear & particles physicsComputer scienceProgramming languagePhysics beyond the Standard ModelFOS: Physical sciencesGeneral Physics and AstronomyPython (programming language)computer.software_genreFile format01 natural sciencesPartícules (Física nuclear)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Hardware and ArchitectureData exchangeInterfacing0103 physical sciencesElectroweak scale010306 general physicscomputercomputer.programming_language
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The see-saw portal at future Higgs Factories

2020

We consider an extension of the Standard Model with two right-handed singlet fermions with mass at the electroweak scale that induce neutrino masses, plus a generic new physics sector at a higher scale $\Lambda$. We focus on the effective operators of lowest dimension $d=5$, which induce new production and decay modes for the singlet fermions. We assess the sensitivity of future Higgs Factories, such as FCC-ee, CLIC-380, ILC and CEPC, to the coefficients of these operators for various center of mass energies. We show that future lepton colliders can test the cut-off of the theory up to $\Lambda \simeq 500 - 1000\;$TeV, surpassing the reach of future indirect measurements of the Higgs and $Z…

High Energy Physics - TheoryNuclear and High Energy PhysicsParticle physicsHiggs PhysicsPhysics beyond the Standard ModelFOS: Physical sciences7. Clean energy01 natural sciencesHigh Energy Physics - ExperimentStandard ModelHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. RadioactivityNeutrino Physics010306 general physicsBeyond Standard Model; Higgs Physics; Neutrino PhysicsPhysics010308 nuclear & particles physicsComputer Science::Information RetrievalHigh Energy Physics::PhenomenologyFermionHigh Energy Physics - PhenomenologyHigh Energy Physics - Theory (hep-th)Beyond Standard ModelHiggs bosonlcsh:QC770-798High Energy Physics::ExperimentCenter of massElectroweak scaleNeutrinoLepton
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DsixTools 2.0: The Effective Field Theory Toolkit

2021

$\tt DsixTools$ is a Mathematica package for the handling of the Standard Model Effective Field Theory (SMEFT) and the Low-energy Effective Field Theory (LEFT) with operators up to dimension six, both at the algebraic and numerical level. $\tt DsixTools$ contains a visually accessible and operationally convenient repository of all operators and parameters of the SMEFT and the LEFT. This repository also provides information concerning symmetry categories and number of degrees of freedom, and routines that allow to implement this information on global expressions (such as decay amplitudes and cross-sections). $\tt DsixTools$ also performs weak basis transformations, and implements the full on…

High Energy Physics - TheoryPhysics and Astronomy (miscellaneous)FOS: Physical scienceslcsh:Astrophysics01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeDimension (vector space)0103 physical scienceslcsh:QB460-466Effective field theorylcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsEngineering (miscellaneous)Quantum chromodynamicsPhysicsBasis (linear algebra)010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)Degrees of freedomRenormalization group3. Good healthAlgebraStandard Model (mathematical formulation)High Energy Physics - PhenomenologyHigh Energy Physics - Theory (hep-th)lcsh:QC770-798Electroweak scale
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Hyperchargeless triplet Majoron model.

1989

We study the general conditions to maintain the scale of the lepton-number-breaking vacuum expectation value at the electroweak scale. It is shown that the only possibilities are if the main component of the resulting Majoron is a hyperchargeless complex triplet or a neutral singlet. Models with a hyperchargeless triplet, even though phenomenologically more interesting, seem to be very difficult to build because they like to break charge conservation. However, we have found a particular extension, by adding an additional neutral singlet, that solves this problem. The model can give a Majorana mass to the neutrinos in the eV range, ..mu -->..e..gamma.. can proceed with branching ratios at th…

Massless particlePhysicsMAJORANAParticle physicsBranching fractionHigh Energy Physics::PhenomenologyElementary particleSinglet stateElectroweak scalePartícules (Física nuclear)Vacuum expectation valueMajoronPhysical review. D, Particles and fields
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Effective field theory after a new-physics discovery

2018

When a new heavy particle is discovered at the LHC or at a future high-energy collider, it will be interesting to study its decays into Standard Model particles using an effective field-theory framework. We point out that the proper effective theory can not be constructed as an expansion in local, higher-dimensional operators; rather, it must be based on non-local operators defined in soft-collinear effective theory (SCET). For the interesting case where the new resonance is a gauge-singlet spin-0 boson, which is the first member of a new sector governed by a mass scale $M$, we show how a consistent scale separation between $M$ and the electroweak scale $v$ is achieved up to next-to-next-to…

Nuclear and High Energy PhysicsParticle physics530 PhysicsPhysics beyond the Standard ModelFOS: Physical sciences10192 Physics Institute01 natural sciencesResonance (particle physics)Standard ModelHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesEffective field theoryRenormalization Grouplcsh:Nuclear and particle physics. Atomic energy. Radioactivity3106 Nuclear and High Energy Physics010306 general physicsBosonPhysics010308 nuclear & particles physicsComputer Science::Information RetrievalHigh Energy Physics::PhenomenologyEffective Field TheoriesRenormalization groupHigh Energy Physics - PhenomenologySoft-collinear effective theoryBeyond Standard Modellcsh:QC770-798ResummationElectroweak scaleJournal of High Energy Physics
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Probes of the Standard Model effective field theory extended with a right-handed neutrino

2019

If neutrinos are Dirac particles and, as suggested by the so far null LHC results, any new physics lies at energies well above the electroweak scale, the Standard Model effective field theory has to be extended with operators involving the right-handed neutrinos. In this paper, we study this effective field theory and set constraints on the different dimension-six interactions. To that aim, we use LHC searches for associated production of light (and tau) leptons with missing energy, monojet searches, as well as pion and tau decays. Our bounds are generally above the TeV for order one couplings. One particular exception is given by operators involving top quarks. These provide new signals in…

Nuclear and High Energy PhysicsParticle physicsPhysics beyond the Standard ModelFOS: Physical sciencesComputer Science::Digital Libraries01 natural sciencesHigh Energy Physics - ExperimentStandard ModelHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesEffective field theoryNeutrino Physicslcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsPhysicsLarge Hadron ColliderMissing energy010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyEffective Field TheoriesNeutrino physicsHigh Energy Physics - PhenomenologyBeyond Standard ModelComputer Science::Mathematical Softwarelcsh:QC770-798High Energy Physics::ExperimentNeutrinoElectroweak scaleLeptonJournal of High Energy Physics
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Dynamical origin of the electroweak scale and the 125 GeV scalar

2015

We consider a fully dynamical origin for the masses of weak gauge bosons and heavy quarks of the Standard Model. Electroweak symmetry breaking and the gauge boson masses arise from new strong dynamics, which leads to the appearance of a composite scalar in the spectrum of excitations. In order to generate mass for the Standard Model fermions, we consider extended gauge dynamics, effectively represented by four fermion interactions at presently accessible energies. By systematically treating these interactions, we show that they lead to a large reduction of the mass of the scalar resonance. Therefore, interpreting the scalar as the recently observed 125 GeV state, implies that the mass origi…

Nuclear and High Energy PhysicsParticle physicsStandard ModelHigh Energy Physics::LatticeSTANDARD MODELFOS: Physical sciencesTechnicolorMASS114 Physical sciences01 natural sciencesSYMMETRY-BREAKINGHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Lattice0103 physical sciencesbeyond-the-Standard-Modellcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsBosonPhysicsGauge bosonta114electroweak symmetry breaking010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)Electroweak interactionHigh Energy Physics::PhenomenologyScalar (physics)BOSONHigh Energy Physics - PhenomenologyHiggs bosonmasslcsh:QC770-798LHCElectroweak scaleScalar fieldNuclear Physics B
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Search for extra dimensions in diphoton events from proton-proton collisions at root s=7 TeV in the ATLAS detector at the LHC

2013

The large difference between the Planck scale and the electroweak scale, known as the hierarchy problem, is addressed in certain models through the postulate of extra spatial dimensions. A search for evidence of extra spatial dimensions in the diphoton channel has been performed using the full set of proton–proton collisions at √s = 7 TeV recorded in 2011 with the ATLAS detector at the CERN Large Hadron Collider. This dataset corresponds to an integrated luminosity of 4.9fb[superscript −1]. The diphoton invariant mass spectrum is observed to be in good agreement with the Standard Model expectation. In the context of the model proposed by Arkani–Hamed, Dimopoulos and Dvali, 95% confidence le…

Particle physicsSignalsGravityGeneral Physics and Astronomyddc:500.201 natural sciencesNuclear physicsElectroweak scale; Planck scale; hierarchy problemContact InteractionsHierarchy0103 physical sciencesColliders[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]CutoffInvariant massddc:530EXTRA DIMENSIONSHierarchy problem010306 general physicsQCPhysicsddc:539Integrated luminosityLarge Hadron ColliderProton proton collisions010308 nuclear & particles physicsAtlas (topology)Parton DistributionsPhysicsSettore FIS/01 - Fisica SperimentaleHigh Energy Physics::PhenomenologyGravitonConfidence levelsFísicaHierarchy problemSpatial dimensionFermion-Pair ProductionCollaborationExtra dimensionsThe standard modelLarge Hadron ColliderInvariant-mass spectraHADRON-HADRON COLLISIONSExperimental High Energy PhysicsComputingMethodologies_DOCUMENTANDTEXTPROCESSINGHigh Energy Physics::ExperimentElectroweak scaleModel
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Composite Higgs bosons from neutrino condensates in an inverted see-saw scenario

2020

We present a realization of the idea that the Higgs boson is mainly a bound state of neutrinos induced by strong four-fermion interactions. The conflicts of this idea with the measured values of the top quark and Higgs boson masses are overcome by introducing, in addition to the right-handed neutrino, a new fermion singlet, which, at low energies, implements the inverse see-saw mechanism. The singlet fermions also develop a scalar bound state which mixes with the Higgs boson. This allows us to obtain a small Higgs boson mass even if the couplings are large, as required in composite scalar scenarios. The model gives the correct masses for the top quark and Higgs boson for compositeness scale…

PhysicsCondensed Matter::Quantum GasesTop quarkParticle physics010308 nuclear & particles physicsHigh Energy Physics::LatticeScalar (mathematics)High Energy Physics::PhenomenologyFOS: Physical sciencesFermion01 natural sciencesPartícules (Física nuclear)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometry0103 physical sciencesHiggs bosonHigh Energy Physics::ExperimentNeutrinoElectroweak scale010306 general physicsBoson
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ICHEP 2014 Summary: Theory Status after the First LHC Run

2016

A brief overview of the main highlights discussed at ICHEP 2014 is presented. The experimental data confirm that the scalar boson discovered at the LHC couples to other particles as predicted in the Standard Model. This constitutes a great success of the present theoretical paradigm, which has been confirmed as the correct description at the electroweak scale. At the same time, the negative searches for signals of new phenomena tightly constrain many new-physics scenarios, challenging previous theoretical wisdom and opening new perspectives in fundamental physics. Fresh ideas are needed to face the many pending questions unanswered within the Standard Model framework.

PhysicsHigh Energy Physics - TheoryNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderStandard Model and Beyond010308 nuclear & particles physicsPhysics beyond the Standard ModelElectroweak interactionFOS: Physical sciencesScalar boson01 natural sciencesStandard ModelHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)0103 physical sciencesFundamental physicsElectroweak and Strong InteractionsHigh Energy PhysicsElectroweak scale010306 general physics
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