Search results for "STANDARD MODEL"

showing 10 items of 1206 documents

Developing the Framed Standard Model

2011

The framed standard model (FSM) suggested earlier, which incorporates the Higgs field and 3 fermion generations as part of the framed gauge theory structure, is here developed further to show that it gives both quarks and leptons hierarchical masses and mixing matrices akin to what is experimentally observed. Among its many distinguishing features which lead to the above results are (i) the vacuum is degenerate under a global $su(3)$ symmetry which plays the role of fermion generations, (ii) the fermion mass matrix is "universal", rank-one and rotates (changes its orientation in generation space) with changing scale $\mu$, (iii) the metric in generation space is scale-dependent too, and in …

Quantum chromodynamicsQuarkPhysicsNuclear and High Energy PhysicsParticle physicsCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesAstronomy and AstrophysicsFermionAtomic and Molecular Physics and OpticsHigh Energy Physics - PhenomenologyStandard Model (mathematical formulation)Higgs fieldTheoretical physicsHigh Energy Physics - Phenomenology (hep-ph)Strong CP problemHigh Energy Physics::ExperimentGauge theory
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Quantum technologies and the elephants

2021

Extraordinary progress in quantum sensors and technologies opens new avenues for exploring the Universe and testing the assumptions forming the basis of modern physics. This QST focus issue: focus on quantum sensors for new-physics discoveries is a next-decade roadmap on developing a wide range of quantum sensors and new technologies towards discoveries of new physics. It covers the next generation of various technologies, including atomic and nuclear clocks, atomic and diamond-based magnetometers, atom and laser interferometers, control of trapped atoms, ions, and molecules, optomechanical systems, and many others. In this editorial, we outline major problems of fundamental physics we aim …

Quantum technologyPhysics and Astronomy (miscellaneous)Emerging technologiesComputer scienceMaterials Science (miscellaneous)Physics beyond the Standard ModelQuantum sensorFundamental physicsPhysics::Atomic PhysicsElectrical and Electronic EngineeringModern physicsEngineering physicsAtomic and Molecular Physics and OpticsQuantum Science and Technology
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Flavour Conservation in Two Higgs Doublet Models

2018

In extensions of the Standard Model with two Higgs doublets, flavour changing Yukawa couplings of the neutral scalars may be present at tree level. In this work we consider the most general scenario in which those flavour changing couplings are absent. We re-analyse the conditions that the Yukawa coupling matrices must obey for such \emph{general flavour conservation} (gFC), and study the one loop renormalisation group evolution of such conditions in both the quark and lepton sectors. We show that gFC in the leptonic sector is one loop stable under the Renormalization Group Evolution (RGE) and in the quark sector we present some new Cabibbo like solution also one loop RGE stable. At a pheno…

QuarkCouplingPhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::LatticeFlavourHigh Energy Physics::PhenomenologyYukawa potentialFOS: Physical sciencesRenormalization group01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Standard Model (mathematical formulation)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHiggs bosonHigh Energy Physics::Experiment010306 general physicsLepton
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Constraining nonstandard neutrino-quark interactions with solar, reactor and accelerator data

2009

We present a reanalysis of nonstandard neutrino-down-quark interactions of electron and tau neutrinos using solar, reactor and accelerator data. In addition updating the analysis by including new solar data from SNO phase III and Borexino, as well as new KamLAND data and solar fluxes, a key role is played in our analysis by the combination of these results with the CHARM data. The latter allows us to better constrain the axial and axial-vector electron and tau-neutrino nonstandard interaction parameters characterizing the deviations from the Standard Model predictions.

QuarkHistoryNuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsPhase (waves)FOS: Physical sciencesElectronEducationStandard ModelPhysics::GeophysicsHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Charm (quantum number)Nuclear Experiment (nucl-ex)Neutrino oscillationNuclear ExperimentSolar and Stellar Astrophysics (astro-ph.SR)BorexinoSolar dataPhysicsNeutral currentHigh Energy Physics::PhenomenologyFísicaComputer Science ApplicationsHigh Energy Physics - PhenomenologyAstrophysics - Solar and Stellar AstrophysicsHigh Energy Physics::ExperimentNeutrino
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Renormalization group invariant matrix elements of Delta S = 2 and Delta I = 3/2 four fermion operators without quark masses

1999

We introduce a new parameterization of four-fermion operator matrix elements which does not involve quark masses and thus allows a reduction of systematic uncertainties. In order to simplify the matching between lattice and continuum renormalization schemes, we express our results in terms of renormalization group invariant B-parameters which are renormalization-scheme and scale independent. As an application of our proposal, matrix elements of DI=3/2 and SUSY DS =2 operators have been computed. The calculations have been performed using the tree-level improved Clover lattice action at two different values of the strong coupling constant (beta=6/g^2=6.0 and 6.2), in the quenched approximati…

QuarkNuclear and High Energy PhysicsHigh Energy Physics::LatticeSTANDARD MODELFOS: Physical sciencesWILSON FERMIONSQuenched approximationPartícules (Física nuclear)kaon decays gauge theory latticeLATTICE QCDRenormalizationHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeKAON B-PARAMETERLattice (order)Mathematical physicsPhysicsHigh Energy Physics - Lattice (hep-lat)FísicaFermionSupersymmetryInvariant (physics)Renormalization groupFIS/02 - FISICA TEORICA MODELLI E METODI MATEMATICIHigh Energy Physics - PhenomenologyHigh Energy Physics::Experiment
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Search for Supersymmetry inppCollisions ats=7  TeVin Events with Two Photons and Missing Transverse Energy

2011

A search for supersymmetry in the context of general gauge-mediated breaking with the lightest neutralino as the next-to-lightest supersymmetric particle and the gravitino as the lightest is presented. The data sample corresponds to an integrated luminosity of 36 pb(-1) recorded by the CMS experiment at the LHC. The search is performed by using events containing two or more isolated photons, at least one hadronic jet, and significant missing transverse energy. No excess of events at high missing transverse energy is observed. Upper limits on the signal cross section for general gauge-mediated supersymmetry between 0.3 and 1.1 pb at the 95% confidence level are determined for a range of squa…

QuarkNuclear and High Energy PhysicsParticle physicsAstrophysics::High Energy Astrophysical PhenomenaGeneral Physics and AstronomyElementary particle01 natural sciencesStandard ModelNuclear physicsHigh Energy Physics::TheoryPionAtlas (anatomy)0103 physical sciencesmedicineNuclear Experiment010306 general physicsPhysicsGluinoLarge Hadron ColliderLuminosity (scattering theory)010308 nuclear & particles physicsHigh Energy Physics::PhenomenologySuperpartnerSupersymmetrymedicine.anatomical_structureNeutralinoHigh Energy Physics::ExperimentGravitinoMinimal Supersymmetric Standard ModelLeptonPhysical Review Letters
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Measurement of the ratio of inclusive cross sectionsσ(pp¯→Z+b−quark jet)/σ(pp¯→Z+jet)ats=1.96  TeV

2005

The ratio of the cross section for $p\bar{p}$ interactions producing a $Z$ boson and at least one $b$ quark jet to the inclusive $Z+{\rm jet}$ cross section is measured using $4.2\ {\rm fb}^{-1}$ of $p\bar{p}$ collisions collected with the \dzero\ detector at the Fermilab Tevatron collider at $\sqrt{s}=1.96$ TeV. The $Z\rightarrow\ell^+\ell^-$ candidate events with at least one $b$ jet are discriminated from $Z+$ charm and light jet(s) events by a novel technique that exploits the properties of the tracks associated to the jet. The measured ratio is $0.0193\pm0.0027$ for events having a jet with transverse momentum $\pt > 20 \GeV$ and pseudorapidity $|\eta| \leq 2.5$, which is the most prec…

QuarkNuclear and High Energy PhysicsParticle physicsAstrophysics::High Energy Astrophysical PhenomenaHadronTevatronGeneral Physics and AstronomyElementary particle7. Clean energy01 natural sciencesBottom quarkStandard Modellaw.inventionNuclear physicslaw0103 physical sciencesNuclear Experiment010306 general physicsColliderBosonPhysicsJet (fluid)Muon010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyPseudorapidityHigh Energy Physics::ExperimentLeptonPhysical Review D
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Measurement of trilinear gauge boson couplings WWV, (V Z,gamma) in e(+)e(-) collisions at 189 GeV

2001

Measurements of the trilinear gauge boson couplings WWgamma and WWZ are presented using the data taken by DELPHI in 1998 at a centre-of-mass energy of 189 GeV and combined with DELPHI data at 183 GeV. Values are determined for Delta(g_1^Z) and Delta(kappa_gamma), the differences of the WWZ charge coupling and of the WWgamma dipole coupling from their Standard Model values, and for lambda_gamma, the WWgamma quadrupole coupling. A measurement of the magnetic dipole and electric quadrupole moment of the W is extracted from the results for Delta(kappa_gamma) and lambda_gamma. The study uses data from the final states jjlv, jjjj, lX, jjX and gammaX, where j represents a quark jet, l an identifie…

QuarkNuclear and High Energy PhysicsParticle physicsENERGIESAstrophysics::High Energy Astrophysical Phenomenastandard modelLEP-IIFOS: Physical sciencesLambda7. Clean energy01 natural sciencesPartícules (Física nuclear)High Energy Physics - ExperimentStandard ModelEVENTSHigh Energy Physics - Experiment (hep-ex)BHABHA SCATTERINGMONTE-CARLO0103 physical sciencesOPTIMAL OBSERVABLES[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]W-MASSgauge couplings010306 general physicsDETECTORQCDELPHIPhysicsGauge boson010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyCharge (physics)LARGE ELECTRON POSITRON COLLIDERFIS/01 - FISICA SPERIMENTALECol·lisions (Física nuclear)QuadrupolePARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHIOPTIMAL OBSERVABLES; BHABHA SCATTERING; MONTE-CARLO; W-MASS; LEP-II; EVENTS; DETECTOR; DELPHI; E+E-->W+W; ENERGIESelectron-positron collisionPARTICLE PHYSICSFísica nuclearHigh Energy Physics::ExperimentE+E-->W+WMagnetic dipoleLepton
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Measurement of the transverse spin correlation in Z → τ+ τ- decays

1997

The measurement of the correlation between the transverse spin components of tau(+)tau(-) pairs collected during 1992 to 1994 with the DELPHI detector at LEP1 is presented. A value C-TT = 0.87 +/- 0.20 (stat.)(-0.12)(+0.10) (syst.) was obtained for the correlation parameter, in agreement with the Standard Model expectation. (C) 1997 Published by Elsevier Science B.V.

QuarkNuclear and High Energy PhysicsParticle physicsLUND MONTE-CARLOElectron–positron annihilationLEP-SLC ENERGIES01 natural sciencesPartícules (Física nuclear)JET FRAGMENTATIONStandard ModelNuclear physicsPHYSICS0103 physical sciencesRADIATIVE-CORRECTIONS010306 general physicsNuclear ExperimentDetectors de radiacióLUND MONTE-CARLO; LEP-SLC ENERGIES; RADIATIVE-CORRECTIONS; JET FRAGMENTATION; TAU-POLARIZATION; SIMULATION; PHYSICS; QUARKSpin-½DELPHIPhysics010308 nuclear & particles physicsTAU-POLARIZATIONQUARKCenter (category theory)LARGE ELECTRON POSITRON COLLIDERTransverse planePARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHISIMULATIONPARTICLE PHYSICSHigh Energy Physics::ExperimentAstrophysics::Earth and Planetary Astrophysics
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The Cabibbo angle as a universal seed for quark and lepton mixings

2015

A model-independent ansatz to describe lepton and quark mixing in a unified way is suggested based upon the Cabibbo angle. In our framework neutrinos mix in a "Bi-Large" fashion, while the charged leptons mix as the "down-type" quarks do. In addition to the standard Wolfenstein parameters (lambda, A) two other free parameters are needed to specify the physical lepton mixing matrix. Through this simple assumption one makes specific predictions for the atmospheric angle as well as leptonic CP violation in good agreement with current observations.

QuarkNuclear and High Energy PhysicsParticle physicsPMNS matrixPhysics beyond the Standard ModelPontecorvo–Maki–Nakagawa–Sakata matrixFOS: Physical sciencesHigh Energy Physics - Phenomenology (hep-ph)ddc:530Mixing (physics)PhysicsCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::PhenomenologyFísicaBi-Large mixinglcsh:QC1-999High Energy Physics - PhenomenologyCKM matrixCabibbo angleCP violationHigh Energy Physics::ExperimentNeutrinoNeutrino mixingWolfenstein parameterlcsh:PhysicsLepton
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