Search results for "STANDARD MODEL"

showing 10 items of 1206 documents

How to discover QCD Instantons at the LHC

2020

Topological Effects in the Standard Model: Instantons, Sphalerons and Beyond at LHC, Geneva, Switzerland, 16 Dec 2020 - 18 Dec 2020; The European physical journal / C 81(7), 624 (2021). doi:10.1140/epjc/s10052-021-09412-1

Particle physicsInstantonp p: scatteringPhysics and Astronomy (miscellaneous)High Energy Physics::LatticeFOS: Physical sciencesquantum [tunneling]QC770-798AstrophysicsComputer Science::Digital Libraries01 natural sciences530Standard Modelvacuum statetopologicalHigh Energy Physics::TheoryCross section (physics)High Energy Physics - Phenomenology (hep-ph)Nuclear and particle physics. Atomic energy. Radioactivityasymmetry [baryon]0103 physical sciencesscattering [p p]ddc:530quantum chromodynamics: instantonLimit (mathematics)010306 general physicsEngineering (miscellaneous)Quantum tunnellingtunneling: quantumQuantum chromodynamicsPhysicsLarge Hadron Colliderelectroweak interaction010308 nuclear & particles physicsHigh Energy Physics::Phenomenologysymmetry breaking: chiralQB460-466High Energy Physics - PhenomenologyCERN LHC Collinstanton [quantum chromodynamics]confinementbaryon: asymmetryComputer Science::Mathematical Softwarechiral [symmetry breaking]Non-perturbativesignature
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Search for diphoton events with large missing transverse energy in 7 TeV proton-proton collisions with the ATLAS detector.

2011

A search for diphoton events with large missing transverse energy is presented. The data were collected with the ATLAS detector in proton-proton collisions at √s=7  TeV at the CERN Large Hadron Collider and correspond to an integrated luminosity of 3.1  pb−1. No excess of such events is observed above the standard model background prediction. In the context of a specific model with one universal extra dimension with compactification radius R and gravity-induced decays, values of 1/R<729  GeV are excluded at 95% C. L., providing the most sensitive limit on this model to date.

Particle physicsMISSING TRANSVERSE ENERGYCiências Naturais::Ciências FísicasAtlas detector:Ciências Físicas [Ciências Naturais]FIS/04 - Fisica Nucleare e SubnucleareGeneral Physics and AstronomyFOS: Physical sciencestransverse energy: missing-energy ; ATLAS ; universal extra dimension ; compactification ; CERN LHC Coll ; background ; p p: interaction ; final state: two-photon ; photon: Kaluza-Klein ; electroweak interaction: standard model: validity test ; experimental results ; 7000 GeV-cmsddc:500.201 natural sciences7. Clean energy530High Energy Physics - ExperimentNuclear physicsUniversal extra dimensionHigh Energy Physics - Experiment (hep-ex)0103 physical sciencesddc:550[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]diphoton; events; transverse energy;proton-proton collisions; Hadron;ddc:530High Energy PhysicsSpecific model010306 general physicsNuclear ExperimentGeneralLiterature_REFERENCE(e.g.dictionariesencyclopediasglossaries)QCPhysicsLarge Hadron ColliderScience & TechnologyCompactification (physics)010308 nuclear & particles physicsAtlas (topology)Settore FIS/01 - Fisica SperimentaleFísicaFIS/01 - Fisica SperimentaleATLASTransverse planeCol·lisions (Física nuclear)Experimental High Energy PhysicsUniversal Extra DimensionsFísica nuclearHigh Energy Physics::ExperimentLHCParticle Physics - ExperimentPhysical review letters
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Search for Supersymmetry with Gauge-Mediated Breaking in Diphoton Events with Missing Transverse Energy at CDF II

2010

8 páginas, 3 figuras.-- PACS numbers: 12.60.Jv, 13.85.Rm, 13.85.Qk, 14.80.Ly.-- CDF Collaboration: et al.

Particle physicsMODELSFOS: Physical sciencesGeneral Physics and Astronomyddc:500.2GAMMA PRODUCTIONKinetic energy114 Physical sciencesE(+)E(-) COLLISIONS; HADRON COLLIDERS; GAMMA PRODUCTION; QCD CORRECTIONS; PHOTON; COUPLINGS; PHYSICS; MODELS; TEV01 natural sciencesHigh Energy Physics - ExperimentStandard ModelPHYSICSNuclear physicsHigh Energy Physics - Experiment (hep-ex)E(+)E(-) COLLISIONS0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Grand Unified TheoryHADRON COLLIDERSSymmetry breakingQuantum field theory010306 general physicsPhysics010308 nuclear & particles physicsPhysicsHigh Energy Physics::PhenomenologySupersymmetryCOUPLINGSTransverse planePHOTONTEVHigh Energy Physics::ExperimentGravitinoQCD CORRECTIONS13.85.Rm 12.60.Jv 13.85.Qk 14.80.Ly
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Observational signatures of Higgs inflation

2016

We investigate the dependency of Higgs inflation on the non-renormalisable matching between the low energy Standard Model limit and the inflationary regime at high energies. We show that for the top mass range $m_t \gtrsim 171.8$ GeV the scenario robustly predicts the spectral index $n_s \simeq 0.97$ and the tensor-to-scalar ratio $r\simeq 0.003$. The matching is however non-trivial, even the best-fit values $m_h=125.09$ GeV and $m_t=173.21$ GeV require a jump $\delta \lambda \sim 0.01$ in the Higgs coupling below the inflationary scale. For $m_t\lesssim 171.8$ GeV, the matching may generate a feature in the inflationary potential. In this case the predicted values of $n_s$ and $r$ vary but…

Particle physicsMatching (statistics)Cosmology and Nongalactic Astrophysics (astro-ph.CO)STANDARD MODELFOS: Physical sciencesAstrophysics::Cosmology and Extragalactic Astrophysics114 Physical sciences01 natural sciencesStandard ModelHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesphysics of the early universeinflationELECTROWEAK VACUUM010306 general physicscosmology of theories beyond the SMBosonInflation (cosmology)PhysicsSpectral index010308 nuclear & particles physicsINDUCED GRAVITY INFLATIONHigh Energy Physics::PhenomenologySpectral densityBOSONAstronomy and Astrophysics115 Astronomy Space scienceHigh Energy Physics - Phenomenologyparticle physics - cosmology connectionJumpHiggs bosonHigh Energy Physics::ExperimentAstrophysics - Cosmology and Nongalactic Astrophysics
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Neutrinoless Double-Electron Capture

2020

Double-beta processes play a key role in the exploration of neutrino and weak interaction properties, and in the searches for effects beyond the Standard Model. During the last half century many attempts were undertaken to search for double-beta decay with emission of two electrons, especially for its neutrinoless mode ($0\nu2\beta^-$), the latter being still not observed. Double-electron capture (2EC) was not in focus so far because of its in general lower transition probability. However, the rate of neutrinoless double-electron capture ($0\nu2$EC) can experience a resonance enhancement by many orders of magnitude in case the initial and final states are energetically degenerate. In the re…

Particle physicsNuclear TheoryAtomic Physics (physics.atom-ph)Electron capturePhysics beyond the Standard ModelFOS: Physical sciencesdouble beta decayGeneral Physics and Astronomyhiukkasfysiikka7. Clean energy01 natural sciencesResonance (particle physics)neutrinoless double beta decayPhysics - Atomic PhysicsNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesNuclear MatrixRoad mapNuclear Experiment (nucl-ex)010306 general physicsNuclear theoryNuclear Experimentnuclear tests of fundamental interactionsPhysics010308 nuclear & particles physicsBeta DecayBolometersHigh Energy Physics - PhenomenologyPräzisionsexperimente - Abteilung BlaumNeutrinoydinfysiikka
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Short-range neutrinoless double beta decay mechanisms

2018

Neutrinoless double beta decay can significantly help to shed light on the issue of non-zero neutrino mass, as observation of this lepton number violating process would imply neutrinos are Majorana particles. However, the underlying interaction does not have to be as simple as the standard neutrino mass mechanism. The entire variety of neutrinoless double beta decay mechanisms can be approached effectively. In this work we focus on a theoretical description of short-range effective contributions to neutrinoless double beta decay, which are equivalent to 9-dimensional effective operators incorporating the appropriate field content. We give a detailed derivation of the nuclear matrix elements…

Particle physicsNuclear TheoryField (physics)Physics beyond the Standard Modeldouble beta decayFOS: Physical sciencesElectron01 natural sciencesneutrinoless double beta decayNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)Double beta decay0103 physical sciences010306 general physicsPhysicsta114electroweak interaction010308 nuclear & particles physicsneutrino interactionsHigh Energy Physics::PhenomenologyForm factor (quantum field theory)3. Good healthHigh Energy Physics - PhenomenologyMAJORANAelectroweak interactions in nuclear physicsPhase spaceHigh Energy Physics::ExperimentNeutrinoPhysical Review D
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Maximal Flavour Violation: a Cabibbo mechanism for leptoquarks

2018

We propose a mechanism that allows for sizeable flavour violation in quark-lepton currents, while suppressing flavour changing neutral currents in quark-quark and lepton-lepton sectors. The mechanism is applied to the recently proposed 4321 renormalizable model, which can accommodate the current experimental anomalies in $B$-meson decays, both in charged and neutral currents, while remaining consistent with all other indirect flavour and electroweak precision measurements and direct searches at high-$p_T$. To support this claim, we present an exhaustive phenomenological survey of this fully calculable UV complete model and highlight the rich complementarity between indirect and direct searc…

Particle physicsNuclear and High Energy Physics530 PhysicsHigh Energy Physics::LatticeFlavourFOS: Physical sciences10192 Physics Institute01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHeavy Quark Physicslcsh:Nuclear and particle physics. Atomic energy. Radioactivity3106 Nuclear and High Energy Physics010306 general physicsParticle Physics - PhenomenologyPhysicshep-ex010308 nuclear & particles physicsComputer Science::Information RetrievalElectroweak interactionHigh Energy Physics::Phenomenologyhep-phComplementarity (physics)High Energy Physics - PhenomenologyGauge SymmetryBeyond Standard Modellcsh:QC770-798High Energy Physics::ExperimentParticle Physics - ExperimentBeyond Standard Model; Gauge Symmetry; Heavy Quark Physics
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Measurement of the ZZ cross-section in e(+)e(-) interactions at 183-189 GeV

2001

Measurements of on-shell ZZ production are described, using data collected by DELPHI in 1997 and 1998, at centre-of-mass energies sqrt(s) = 182.6 GeV and 188.6 GeV respectively. Results obtained in each of the final states q qbar q qbar, mu+mu- q qbar, e+e- q qbar, nu nubar q qbar, l+l-l+l-, and nu nubar l+l- are presented. The measured cross-sections for on-shell ZZ production via the tree-level doubly-resonant graphs (NC02) are: sigma_{NC02}(182.6 GeV) = 0.38 +- 0.18 (stat) +- 0.04 (syst) pb, sigma_{NC02}(188.6 GeV) = 0.60 +- 0.13 (stat) +- 0.07 (syst) pb. They are consistent with the Standard Model expectations of 0.25 pb and 0.65 pb at each energy.

Particle physicsNuclear and High Energy PhysicsCOLLISIONSLOWEST ORDER CALCULATIONSPAIR PRODUCTIONENERGIESMONTE-CARLO SIMULATIONFOS: Physical sciences2-PHOTON PROCESSES01 natural sciencesPartícules (Física nuclear)Standard ModelHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)LEP2SEARCH0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]PROGRAM010306 general physicsQCDELPHIPhysics010308 nuclear & particles physicsPhysicsSigmaMONTE-CARLO SIMULATION; LOWEST ORDER CALCULATIONS; PAIR PRODUCTION; 2-PHOTON PROCESSES; ROOT-S=183 GEV; COLLISIONS; PROGRAM; LEP2; ENERGIES; SEARCHLARGE ELECTRON POSITRON COLLIDERPARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHIPARTICLE PHYSICSFísica nuclearParticle Physics - ExperimentROOT-S=183 GEV
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Hunt for new phenomena using large jet multiplicities and missing transverse momentum with ATLAS in 4.7 fb[superscript −1] of √s = 7 TeV proton-proto…

2012

Results are presented of a search for new particles decaying to large numbers of jets in association with missing transverse momentum, using 4.7 fb[superscript −1] of pp collision data at √s = 7 TeV collected by the ATLAS experiment at the Large Hadron Collider in 2011. The event selection requires missing transverse momentum, no isolated electrons or muons, and from ≥6 to ≥9 jets. No evidence is found for physics beyond the Standard Model. The results are interpreted in the context of a MSUGRA/CMSSM supersymmetric model, where, for large universal scalar mass m [subscript 0], gluino masses smaller than 840 GeV are excluded at the 95% confidence level, extending previously published limits.…

Particle physicsNuclear and High Energy PhysicsCiências Naturais::Ciências FísicasPhysics beyond the Standard Model:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.201 natural sciences7. Clean energy530High Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]ddc:530High Energy Physics010306 general physicsNuclear ExperimentCiencias ExactasPhysicsddc:539GluinoLarge Hadron ColliderHadron-Hadron ScatteringScience & Technology010308 nuclear & particles physicsProton-proton collisionATLAS experimentSettore FIS/01 - Fisica SperimentaleHigh Energy Physics::PhenomenologyFísicaSupersymmetryATLASHadron-Hadron scatteringLarge Hadron ColliderHADRON-HADRON COLLISIONSNeutralinoHigh Energy Physics::ExperimentLHCParticle Physics - ExperimentMinimal Supersymmetric Standard ModelLepton
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Baryogenesis through split Higgsogenesis

2013

We study the cosmological evolution of asymmetries in the two-Higgs doublet extension of the Standard Model, prior to the electroweak phase transition. If Higgs flavour-exchanging interactions are sufficiently slow, then a relative asymmetry among the Higgs doublets corresponds to an effectively conserved quantum number. Since the magnitude of the Higgs couplings depends on the choice of basis in the :Higgs doublet space, we attempt to formulate basis-independent out-of-equilibrium conditions. We show that an initial asymmetry between the fliggs scalars, which could be generated by GP violation in the :Higgs sector, will be transformed into a baryon asymmetry by the sphalerons, without the …

Particle physicsNuclear and High Energy PhysicsHiggs Physicsmedia_common.quotation_subjectHigh Energy Physics::LatticeFOS: Physical sciences01 natural sciencesAsymmetryStandard ModelHiggs sectorBaryon asymmetryHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsmedia_commonPhysics010308 nuclear & particles physicsElectroweak interactionHigh Energy Physics::PhenomenologyFísicaBaryogenesisHigh Energy Physics - PhenomenologyCP violation[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Higgs bosonCP violationHigh Energy Physics::ExperimentJournal of High Energy Physics
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