Search results for "symmetries"

showing 10 items of 84 documents

Hemispheric differences in specificity effects in talker identification

2010

In the visual domain, Marsolek and colleagues (1999, 2008) have found support for two dissociable and parallel neural subsystems underlying object and shape recognition: an abstract-category subsystem that operates more effectively in the left cerebral hemisphere (LH), and a specific-exemplar subsystem that operates more effectively in the right cerebral hemisphere (RH). Evidence of this asymmetry has been observed in priming specificity for linguistic (words, pseudoword forms) and nonlinguistic (objects) stimuli. In the auditory domain, the authors previously found hemispheric asymmetries in priming effects for linguistic (spoken words) and nonlinguistic (environmental sounds) stimuli. In …

Linguistics and Languagemedicine.medical_specialtyProperty (programming)Cervell--Localització de funcionsmedia_common.quotation_subjectObject (grammar)Experimental and Cognitive PsychologyAudiologyLanguage and LinguisticsPerceptionmedicineHumansDominance Cerebralmedia_commonCommunicationbusiness.industryHemisphere asymmetriesReconeixement de la parlaTalker identificationSensory SystemsSemanticsPseudowordAcoustic StimulationPattern Recognition VisualPrimingLateralitySpeech PerceptionTest phaseIdentification (psychology)Specificity effectsCuesPsychologybusinessPriming (psychology)Attention, Perception, & Psychophysics
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Electroweak breaking and neutrino mass

2017

En este trabajo de tesis hemos analizado algunas de las posibles conexiones entre la generación de la masa de los neutrinos y la nueva física. Para ello, como preámbulo, en el primer capítulo hemos hecho un repaso del Modelo Estándar (SM) de la física de partículas, siendo ésta la descripción más precisa que tenemos de las las interacciones fuertes, débiles y electromagnéticas. Sin embargo, existen algunas interrogantes a las que el SM no ofrece respuesta, por ejemplo, ¿Por qué hay tres familias de quarks y leptones?, ¿Cuál es la explicación a la jerarquía de las masas de los fermiones y a sus ángulos de mezcla?, ¿Cómo explicar la jerarquía entre la escala electrodébil y la escala de Planck…

Neutrino massneutrino natureHiggs propertiesdark matterFlavour symmetries
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Transverse Beam Spin Asymmetries at Backward Angles in Elastic Electron-Proton and Quasielastic Electron-Deuteron Scattering

2011

We have measured the beam-normal single-spin asymmetries in elastic scattering of transversely polarized electrons from the proton, and performed the first measurement in quasi-elastic scattering on the deuteron, at backward angles (lab scattering angle of 108 degrees) for Q2 = 0.22 GeV^2/c^2 and 0.63 GeV^2/c^2 at beam energies of 362 MeV and 687 MeV, respectively. The asymmetry arises due to the imaginary part of the interference of the two-photon exchange amplitude with that of single photon exchange. Results for the proton are consistent with a model calculation which includes inelastic intermediate hadronic (piN) states. An estimate of the beam-normal single-spin asymmetry for the scatt…

Nuclear TheoryNuclear TheoryGeneral Physics and Astronomyaxial-vector currentFOS: Physical sciencesInelastic scatteringMott scattering[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]strange quark01 natural sciencesNuclear physicsNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)parity-violating asymmetries; axial-vector current; strange quark; charge and magnetic nucleon form factors0103 physical sciencesNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentElastic scatteringPhysicsQuasielastic scattering010308 nuclear & particles physicsScatteringcharge and magnetic nucleon form factorsparity-violating asymmetriesSmall-angle neutron scatteringNATURAL SCIENCES. Physics.PRIRODNE ZNANOSTI. Fizika.High Energy Physics - PhenomenologyQuasielastic neutron scatteringPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentScattering theoryAtomic physics
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Meson Resonances at large Nc: Complex Poles vs Breit-Wigner Masses

2009

The rigorous quantum mechanical definition of a resonance requires determining the pole position in the second Riemann sheet of the analytically continued partial wave scattering amplitude in the complex Mandelstam s variable plane. For meson resonances we investigate the alternative Breit–Wigner (BW) definition within the large NC expansion. By assuming that the pole position is View the MathML source and exploiting unitarity, we show that the BW determination of the resonance mass differs from the pole position by View the MathML source terms, which can be extracted from ππ scattering data. For the case of the σ (f0(600)) pole, the BW scalar mass is predicted to occur at not, vert, simila…

Nuclear and High Energy PhysicsMesonScalar (mathematics)FOS: Physical sciences01 natural sciencesUnitarizationHigh Energy Physics - Phenomenology (hep-ph)Quantum mechanics0103 physical sciences010306 general physicsScalar mesonChiral symmetriesScalar mesonPhysicsUnitarity010308 nuclear & particles physicsPlane (geometry)ScatteringLarge N-CResonanceFísicaScattering amplitudeHigh Energy Physics - PhenomenologyResonancesQuantum electrodynamics
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A search for neutron to mirror-neutron oscillations using the nEDM apparatus at PSI

2021

It has been proposed that there could be a mirror copy of the standard model particles, restoring the parity symmetry in the weak interaction on the global level. Oscillations between a neutral standard model particle, such as the neutron, and its mirror counterpart could potentially answer various standing issues in physics today. Astrophysical studies and terrestrial experiments led by ultracold neutron storage measurements have investigated neutron to mirror-neutron oscillations and imposed constraints on the theoretical parameters. Recently, further analysis of these ultracold neutron storage experiments has yielded statistically significant anomalous signals that may be interpreted as …

Nuclear and High Energy PhysicsNeutron electric dipole momentmedia_common.quotation_subjectmagnetic fieldWeak interaction[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Astronomy & Astrophysics01 natural sciences7. Clean energyAsymmetryrotationPhysics Particles & FieldsELECTRIC-DIPOLE MOMENTweak interaction0103 physical sciencesDark matterDARK-MATTERNeutron010306 general physicsnumerical calculationsmirrorNuclear mattermedia_commonoscillation: timePhysicsn: electric momentProperties of neutrons Ultracold neutrons Nuclear matter Mirror matter Dark matter Particle symmetriesScience & TechnologyProperties of neutronsParticle symmetries010308 nuclear & particles physicsparity: symmetryPhysicsNuclear matter[PHYS.PHYS.PHYS-GEN-PH]Physics [physics]/Physics [physics]/General Physics [physics.gen-ph]lcsh:QC1-999Mirror matterMagnetic fieldMODELPhysics Nuclear[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Physical SciencesUltracold neutronsAtomic physicsUltracold neutronsMirror matterasymmetrylcsh:PhysicsPhysics Letters B
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On the strength of the U A (1) anomaly at the chiral phase transition in N f = 2 QCD

2016

We study the thermal transition of QCD with two degenerate light flavours by lattice simulations using $O(a)$-improved Wilson quarks. Temperature scans are performed at a fixed value of $N_t = (aT)^{-1}=16$, where $a$ is the lattice spacing and $T$ the temperature, at three fixed zero-temperature pion masses between 200 MeV and 540 MeV. In this range we find that the transition is consistent with a broad crossover. As a probe of the restoration of chiral symmetry, we study the static screening spectrum. We observe a degeneracy between the transverse isovector vector and axial-vector channels starting from the transition temperature. Particularly striking is the strong reduction of the split…

Nuclear and High Energy PhysicsNuclear TheorySpontaneous symmetry breakingHigh Energy Physics::LatticeNuclear TheoryFOS: Physical sciences01 natural sciencesNuclear Theory (nucl-th)PionHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsMass screeningPhysicsQuantum chromodynamicsIsovectorCondensed matter physics010308 nuclear & particles physicsTransition temperatureMESON SCREENING MASSES; HIGH-TEMPERATURE PHASE; QUARK-GLUON PLASMA; LATTICE QCD; WILSON FERMIONS; HADRONIC SPECTRUM; O(A) IMPROVEMENT; U(1)(A) SYMMETRY; GAUGE-THEORIES; STRANGE QUARK; Global Symmetries; Lattice QCD; Phase Diagram of QCD; Spontaneous Symmetry BreakingHigh Energy Physics - Lattice (hep-lat)ddc:530Lattice QCD530 PhysikPseudoscalarHigh Energy Physics - Phenomenology
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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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Updated BBN bounds on the cosmological lepton asymmetry for non-zero 13

2011

We discuss the bounds on the cosmological lepton number from Big Bang Nucleosynthesis (BBN), in light of recent evidences for a large value of the neutrino mixing angle theta13. The largest asymmetries for electron and muon or tau neutrinos compatible with 4He and 2H primordial yields are computed versus the neutrino mass hierarchy and mixing angles. The flavour oscillation dynamics is traced till the beginning of BBN and neutrino distributions after decoupling are numerically computed. The latter contains in general, non thermal distortion due to the onset of flavour oscillations driven by solar squared mass difference in the temperature range where neutrino scatterings become inefficient …

Nuclear and High Energy PhysicsParticle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)media_common.quotation_subjectAstrophysics::High Energy Astrophysical PhenomenaPhysics of the early UniverseFOS: Physical sciences01 natural sciencesAsymmetryPartícules (Física nuclear)symbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)Big Bang nucleosynthesis0103 physical sciencesPrimordial asymmetriesPlanckNeutrinos010306 general physicsNeutrino oscillationmedia_commonPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyDecoupling (cosmology)Lepton numberHigh Energy Physics - PhenomenologysymbolsHigh Energy Physics::ExperimentNeutrinoLeptonAstrophysics - Cosmology and Nongalactic Astrophysics
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Searches for violation of lepton flavour and baryon number in tau lepton decays at LHCb

2013

Searches for the lepton flavour violating decay tau(-) -> mu(-)mu(+)mu(-) and the lepton flavour and baryon number violating decays tau(-) -> (p) over bar mu(+)mu(-) and tau(-) -> p mu(-)mu(-) have been carried out using proton-proton collision data, corresponding to an integrated luminosity of 1.0 fb(-1), taken by the LHCb experiment at root s = 7 TeV. No evidence has been found for any signal, and limits have been set at 90% confidence level on the branching fractions: B(tau(-) -> mu(-)mu(+)mu(-) mu(+)mu(-)) p mu(-)mu(-)) (p) over bar mu(+)mu(-) and tau(-) -> p mu(-)mu(-) decay modes represent the first direct experimental limits on these channels.

Nuclear and High Energy PhysicsParticle physicsFlavourDecays of leptons; Global symmetries (e.g. baryon number lepton number); 13.35.-r; 11.30.Fs;FOS: Physical sciences01 natural sciencesPartícules (Física nuclear)High Energy Physics - ExperimentSettore FIS/04 - Fisica Nucleare e SubnucleareNuclear physicslepton number)High Energy Physics - Experiment (hep-ex)Violació CP (Física nuclear)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]LHC flavour physics lepton number11.30.FsNeutrinsNeutrinos010306 general physicsParticles (Nuclear physics)Physics13.35.-rDecays of leptonsLarge Hadron Collider010308 nuclear & particles physicsGlobal symmetries (e.g. baryon number lepton number)Leptons (Física nuclear)Global symmetries (e.g.High Energy Physics::Phenomenologybaryon numberDecays of lepton3. Good healthFIS/01 - FISICA SPERIMENTALELeptons (Nuclear physics)Física nuclearHigh Energy Physics::ExperimentBaryon numberNeutrino11.30.FFIS/04 - FISICA NUCLEARE E SUBNUCLEAREParticle Physics - ExperimentLeptonCP violation (Nuclear physics)Physics Letters B
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Neutrino phenomenology and stable dark matter with A4

2011

We present a model based on the A4 non-abelian discrete symmetry leading to a predictive five-parameter neutrino mass matrix and providing a stable dark matter candidate. We found an interesting correlation among the atmospheric and the reactor angles which predicts theta_23 ~ pi/4 for very small reactor angle and deviation from maximal atmospheric mixing for large theta_13. Only normal neutrino mass spectrum is possible and the effective mass entering the neutrinoless double beta decay rate is constrained to be |m_ee| > 4 10^{-4} eV.

Nuclear and High Energy PhysicsParticle physicsLepton mixingDark matterDiscrete symmetriesFOS: Physical sciencesElementary particle01 natural sciences7. Clean energyNuclear physicsEffective mass (solid-state physics)High Energy Physics - Phenomenology (hep-ph)Double beta decay0103 physical sciencesDark matterNeutrinoless double beta decay010306 general physicsNeutrino oscillationPhysics010308 nuclear & particles physicsFlavor symmetriesNeutrino massesMassless particleHigh Energy Physics - PhenomenologyMass spectrumNeutrinoPhysics Letters B
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