Search results for "Particle physics"

showing 10 items of 6826 documents

A search for invisible Higgs bosons produced in e+e- interactions at LEP 2 energies

1999

Searches for HZ production with the Higgs boson decaying into an invisible final state have been performed with the data collected by the DELPHI experiment up to the centre-of-mass energy of 183 GeV. The hadronic and muon pair final states of the Z boson were analysed. From the absence of signal, upper limits on the cross-section and the corresponding Higgs boson mass limits were set at 95% confidence level. The results are interpreted as excluded parameter regions in the framework of the minimal supersymmetric standard model and in the simplest Majoron model with one Higgs doublet and one Higgs singlet field. (C) 1999 Elsevier Science B.V. All rights reserved.

Nuclear and High Energy PhysicsParticle physicsCOLLISIONSVIOLATIONSTANDARD MODELMASS01 natural sciencesDECAYSPartícules (Física nuclear)Standard ModelNuclear physicsPHYSICSsymbols.namesakeMONTE-CARLO0103 physical sciencesPROGRAM[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]STANDARD MODEL; MONTE-CARLO; PHYSICS; DECAYS; PROGRAM; SUPERSYMMETRY; COLLISIONS; VIOLATION; PARTICLE; MASS010306 general physicsSUPERSYMMETRYBosonMajoronDELPHIPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologySupersymmetryLARGE ELECTRON POSITRON COLLIDERHiggs fieldPARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHIsymbolsHiggs bosonPARTICLE PHYSICSFísica nuclearHigh Energy Physics::ExperimentPARTICLEHiggs mechanismParticle Physics - ExperimentMinimal Supersymmetric Standard Model
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Transverse spin effects in hadron-pair production from semi-inclusive deep inelastic scattering

2012

First measurements of azimuthal asymmetries in hadron-pair production in deep-inelastic scattering of muons on transversely polarised ^6LiD (deuteron) and NH_3 (proton) targets are presented. The data were taken in the years 2002-2004 and 2007 with the COMPASS spectrometer using a muon beam of 160 GeV/c at the CERN SPS. The asymmetries provide access to the transversity distribution functions, without involving the Collins effect as in single hadron production. The sizeable asymmetries measured on the NH_ target indicate non-vanishing u-quark transversity and two-hadron interference fragmentation functions. The small asymmetries measured on the ^6LiD target can be interpreted as indication …

Nuclear and High Energy PhysicsParticle physicsCOMPASS; SIDIS; two hadron azimuthal asymmetries; transversityHadronNuclear TheoryFOS: Physical sciencesCOMPASSSIDIS01 natural sciencesHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciences010306 general physicsNuclear ExperimenttransversityPhysicsLarge Hadron ColliderMuonSpectrometerta114010308 nuclear & particles physicsScatteringtwo hadron azimuthal asymmetrietwo hadron azimuthal asymmetriesHigh Energy Physics::PhenomenologyDeep inelastic scatteringPair productionDistribution functionHigh Energy Physics::ExperimentParticle Physics - ExperimentPhysics Letters B
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Neutrinos, DUNE and the world best bound on CPT invariance

2017

CPT symmetry, the combination of Charge Conjugation, Parity and Time reversal, is a cornerstone of our model building strategy and therefore the repercussions of its potential violation will severely threaten the most extended tool we currently use to describe physics, i.e. local relativistic quantum fields. However, limits on its conservation from the Kaon system look indeed imposing. In this work we will show that neutrino oscillation experiments can improve this limit by several orders of magnitude and therefore are an ideal tool to explore the foundations of our approach to Nature. Strictly speaking testing CPT violation would require an explicit model for how CPT is broken and its effe…

Nuclear and High Energy PhysicsParticle physicsCPT symmetryFOS: Physical sciences01 natural sciencesPartícules (Física nuclear)High Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsNeutrino oscillationQuantumPhysics010308 nuclear & particles physicsOscillationHigh Energy Physics::PhenomenologyParity (physics)Observablelcsh:QC1-999High Energy Physics - PhenomenologyHigh Energy Physics::ExperimentNeutrinoModel buildinglcsh:Physics
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Odd parity bottom-flavored baryon resonances

2013

The LHCb Collaboration has recently observed two narrow baryon resonances with beauty. Their masses and decay modes look consistent with the quark model orbitally excited states Lambda(b)(5912) and Lambda(b)*(5920), with quantum numbers J(P) = 1/2(-) and 3/2(-), respectively. We predict the existence of these states within a unitarized meson-baryon coupled-channel dynamical model, which implements heavy-quark spin symmetry. Masses, quantum numbers and couplings of these resonances to the different meson-baryon channels are obtained. We find that the resonances Lambda(0)(b)(5912) and Lambda(0)(b)(5920) are heavy-quark spin symmetry partners, which naturally explains their approximate mass de…

Nuclear and High Energy PhysicsParticle physicsCharmNuclear TheoryN-asteriskHigh Energy Physics::LatticeNuclear TheoryFOS: Physical sciences01 natural sciencesCHARMNuclear Theory (nucl-th)SUM-RULESHigh Energy Physics - Phenomenology (hep-ph)Heavy-quark symmetryMESON-EXCHANGE0103 physical sciencesChiral dynamicsNuclear Experiment010306 general physicsNuclear theorySpectroscopyKaon-nucleon interactionsPhysicsMeson-exchangeStatesSPECTROSCOPYCoupled-channelN-ASTERISK010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyCHIRAL DYNAMICSFísicaCOUPLED-CHANNELHEAVY-QUARK SYMMETRYHigh Energy Physics - PhenomenologySTATESSum-rulesKAON-NUCLEON INTERACTIONSHigh Energy Physics::ExperimentSpin symmetryHumanities
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Improvement in fast particle track reconstruction with robust statistics

2014

The IceCube project has transformed one cubic kilometer of deep natural Antarctic ice into a Cherenkov detector. Muon neutrinos are detected and their direction inferred by mapping the light produced by the secondary muon track inside the volume instrumented with photomultipliers. Reconstructing the muon track from the observed light is challenging due to noise, light scattering in the ice medium, and the possibility of simultaneously having multiple muons inside the detector, resulting from the large flux of cosmic ray muons. This manuscript describes work on two problems: (1) the track reconstruction problem, in which, given a set of observations, the goal is to recover the track of a muo…

Nuclear and High Energy PhysicsParticle physicsCherenkov detectorPhysics::Instrumentation and DetectorsFOS: Physical sciencesddc:500.2Neutrino telescopeTrack reconstructionlaw.inventionIceCubelawCoincidentAngular resolutionddc:530InstrumentationInstrumentation and Methods for Astrophysics (astro-ph.IM)Remote sensingIce CubePhysicsMuonTrack (disk drive)DetectorIceCube; Neutrino astrophysics; Neutrino telescope; Robust statistics; Track reconstructionRobust statisticsNeutrino astrophysicsNeutrino detectorHigh Energy Physics::ExperimentNeutrinoAstrophysics - Instrumentation and Methods for AstrophysicsNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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A strategy to study the role of the charm quark in explaining the Delta{I}=1/2 rule

2004

We present a strategy designed to separate several possible origins of the well-known enhancement of the Delta{I}=1/2 amplitude in non-leptonic kaon decays. In particular, we seek to disentangle the contribution of physics at the typical QCD scale (soft-gluon exchange) from the effects at the scale of the charm quark mass. This is achieved by considering QCD with an unphysically light charm quark, so that the theory possesses an approximate SU(4)_L x SU(4)_R chiral symmetry. By computing the relevant operator matrix elements and monitoring their values as the charm quark mass departs from the SU(4)-symmetric situation, the role of the charm quark can be assessed. We study the influence of t…

Nuclear and High Energy PhysicsParticle physicsChiral perturbation theoryHigh Energy Physics::LatticeLattice (group)FOS: Physical sciencesScale (descriptive set theory)weak decaysCharm quarkHigh Energy Physics - Phenomenology (hep-ph)lattice QCDHigh Energy Physics - Latticefield theory gauge theory lattice kaon decayskaon physicschiral lagrangiansLimit (mathematics)Quantum chromodynamicsPhysicsHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyFísicaFIS/02 - FISICA TEORICA MODELLI E METODI MATEMATICIHigh Energy Physics - PhenomenologyAmplitudeOperator matrixHigh Energy Physics::Experiment
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Pion and kaon vector form factors

2001

We develop a unitarity approach to consider the final state interaction corrections to the tree level graphs calculated from Chiral Perturbation Theory ($\chi PT$) allowing the inclusion of explicit resonance fields. The method is discussed considering the coupled channel pion and kaon vector form factors. These form factors are then matched with the one loop $\chi PT$ results. A very good description of experimental data is accomplished for the vector form factors and for the $\pi\pi$ P-wave phase shifts up to $\sqrt{s}\lesssim 1.2$ GeV, beyond which multiparticle states play a non negligible role. In particular the low and resonance energy regions are discussed in detail and for the forme…

Nuclear and High Energy PhysicsParticle physicsChiral perturbation theoryNuclear TheoryPartial wave analysisFOS: Physical sciencesPerturbation (astronomy)chiral [perturbation theory]CoincidenceHigh Energy Physics - ExperimentNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Pioninterpretation of experiments [numerical calculations]Dispersion relationtree approximationunitarityddc:530higher-order [Feynman graph]form factor [K]PhysicsUnitarityFísicapartial wave analysisHigh Energy Physics - Phenomenologyform factor [pi]vector [form factor]Quantum electrodynamicsIsospinelastic scattering [pi pi]correction [final-state interaction]
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High-precision determination of the $K_{e3}$ radiative corrections

2021

We report a high-precision calculation of the Standard Model electroweak radiative corrections in the $K\to \pi e^+\nu(\gamma)$ decay as a part of the combined theory effort to understand the existing anomaly in the determinations of $V_{us}$. Our new analysis features a chiral resummation of the large infrared-singular terms in the radiative corrections and a well-under-control strong interaction uncertainty based on the most recent lattice QCD inputs. While being consistent with the current state-of-the-art results obtained from chiral perturbation theory, we reduce the existing theory uncertainty from $10^{-3}$ to $10^{-4}$. Our result suggests that the Standard Model electroweak effects…

Nuclear and High Energy PhysicsParticle physicsChiral perturbation theoryNuclear TheoryQC1-999Strong interactionFOS: Physical sciences01 natural sciencesStandard ModelHigh Energy Physics - ExperimentNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)High Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesRadiative transferddc:530ResummationNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentPhysics010308 nuclear & particles physicsPhysicsElectroweak interactionHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)Lattice QCDHigh Energy Physics - PhenomenologyAnomaly (physics)
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S-wave Kpi scattering in chiral perturbation theory with resonances

2000

32 páginas, 6 figuras, 2 tablas.-- PACS: 11.80.Et; 12.39.Fe; 13.75.Lb; 13.85.Fb.-- arXiv:hep-ph/0006045v1

Nuclear and High Energy PhysicsParticle physicsChiral perturbation theoryNuclear TheoryScalar (mathematics)FOS: Physical sciencesMeson–meson interactionsHigh Energy Physics - ExperimentNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)S-wavePartial-wave analysisddc:530Nuclear Experiment (nucl-ex)Nuclear ExperimentPhysicsScatteringtwo-particle final states [Inelastic scattering]ResonanceFísicaRange (mathematics)High Energy Physics - PhenomenologyUnitarisationInelastic scattering: two-particle final statesChiral lagrangiansEnergy (signal processing)
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On the pion cloud of the nucleon

2003

We evaluate the two--pion contribution to the nucleon electromagnetic form factors by use of dispersion analysis and chiral perturbation theory. After subtraction of the rho--meson component, we calculate the distributions of charge and magnetization in coordinate space, which can be interpreted as the effects of the pion cloud. We find that the charge distribution of this pion cloud effect peaks at distances of about 0.3 fm. Furthermore, we calculate the contribution of the pion cloud to the isovector charges and radii of the nucleon.

Nuclear and High Energy PhysicsParticle physicsChiral perturbation theoryNuclear Theorydispersion relationHigh Energy Physics::LatticeisovectorNuclear Theorychiral [perturbation theory]FOS: Physical sciencestwo-pion [effect]form factor [nucleon]density [charge]Nuclear physicsNuclear Theory (nucl-th)PionHigh Energy Physics - Phenomenology (hep-ph)ddc:530Perturbation theoryCoordinate spacenumerical calculationsNuclear ExperimentPhysicsIsovectorpole [rho(770)]Charge densityCharge (physics)High Energy Physics - Phenomenologycloud [pi]High Energy Physics::Experimentspectral representationNucleon
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