Search results for "UNITARITY"

showing 10 items of 245 documents

Non-Unitarity of the lepton mixing matrix at the European spallation source

2022

If neutrinos get mass through the exchange of lepton mediators, as in seesaw schemes, the neutrino appearance probabilities in oscillation experiments are modified due to effective nonunitarity of the lepton mixing matrix. This also leads to new CP phases and an ambiguity in underpinning the ''conventional'' phase of the three-neutrino paradigm. We study the CP sensitivities of various setups based at the European spallation source neutrino super-beam (ESSnuSB) experiment in the presence of nonunitarity. We also examine its potential in constraining the associated new physics parameters. Moreover, we show how the combination of DUNE and ESSnuSB can help further improve the sensitivities on …

PMNS matrixPhysics::Instrumentation and Detectorsnew physicsHigh Energy Physics::Phenomenologyphase: CPFOS: Physical scienceslepton: mixingneutrino: mixing angleHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)ESSnuSB[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]CP: violation[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]High Energy Physics::Experimentneutrino: oscillationunitarity: violation
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Asymptotic properties of Born-improved amplitudes with gauge bosons in the final state

1999

For processes with gauge bosons in the final state we show how to continuously connect with a single Born-improved amplitude the resonant region, where resummation effects are important, with the asymptotic region far away from the resonance, where the amplitude must reduce to its tree-level form. While doing so all known field-theoretical constraints are respected, most notably gauge-invariance, unitarity and the equivalence theorem. The calculations presented are based on the process $f\bar{f}\to ZZ$, mediated by a possibly resonant Higgs boson; this process captures all the essential features, and can serve as a prototype for a variety of similar calculations. By virtue of massive cancel…

PhysicsNuclear and High Energy PhysicsGauge bosonParticle physicsUnitarityHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaState (functional analysis)Resonance (particle physics)RenormalizationHigh Energy Physics - PhenomenologyAmplitudeHigh Energy Physics - Phenomenology (hep-ph)Higgs bosonResummationMathematical physicsParticle Physics - Phenomenology
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Quantum loops in radiative decays of the a1 and b1 axial-vector mesons

2007

A previous model where the low-lying axial-vector mesons are dynamically generated, implementing unitarity in coupled channels in the vector-pseudoscalar (V P) meson interaction, is applied to evaluate the decay widths of the a1(1260) and b1(1235) axial-vector mesons into �. Unlike the case of the a1, the b1 radiative decay is systematically underestimated at tree level. In this work we evaluate for the first time the loop contribution coming from an initial V P vertex. Despite the large superficial divergence of the loops, the convergence of the relevant loops can be established by using arguments of gauge invariance. The partial decay widths obtained agree with the experimental values wit…

PhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryUnitarityMesonQuantum electrodynamicsRadiative transferGauge theoryPseudovectorQuantumVertex (geometry)Physics Letters B
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Tree-level flavor-changing neutral currents in theBsystem: FromCPasymmetries to rare decays

2001

corresponding to 0.59 ≤ sin(2�) ≤ 0.82, which is cer- tainly outside the 1� Babar range but not outside the world average. This potential discrepancy is at the ori- gin of several papers (6) studying the implications of a small aJ/ in the search of new physics. In this paper, we analyze the implications of this situ- ation for a realistic model, obtained with the only addi- tion of an isosinglet down vector-like quark (7) to the SM spectrum. This model naturally arises, for instance, as the low-energy limit of an E6 grand unified theory. At a more phenomenological level, models with isosinglet quarks provide the simplest self-consistent framework to study deviations of 3 ×3 unitarity of the…

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsUnitarityCabibbo–Kobayashi–Maskawa matrixPhysics beyond the Standard ModelGrand Unified TheoryB mesonQuarkoniumStandard ModelPhysical Review D
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Massive Yang-Mills model and diffractive scattering

1998

We argue that the massive Yang-Mills model of Kunimasa and Goto, Slavnov, and Cornwall, in which massive gauge vector bosons are introduced in a gauge-invariant way without resorting to the Higgs mechanism, may be useful for studying diffractive scattering of strongly interacting particles. We perform in this model explicit calculations of S-matrix elements between quark states, at tree level, one loop, and two loops, and discuss issues of renormalisability and unitarity. In particular, it is shown that the S-matrix element for quark scattering is renormalisable at one-loop order and is only logarithmically non-renormalisable at two loops. The discrepancies in the ultraviolet regime between…

QuarkPhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsUnitarityHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaGluonsymbols.namesakePomeronHigh Energy Physics - PhenomenologyHigh Energy Physics::TheoryHigh Energy Physics - Phenomenology (hep-ph)symbolsHigh Energy Physics::ExperimentHiggs mechanismParticle Physics - PhenomenologyS-matrixBoson
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Higgs Pair Production as a Signal of Enhanced Yukawa Couplings

2018

We present a non-trivial correlation between the enhancement of the Higgs-fermion couplings and the Higgs pair production cross section in two Higgs doublet models with a flavour symmetry. This symmetry suppresses flavour-changing neutral couplings of the Higgs boson and allows for a partial explanation of the hierarchy in the Yukawa sector. After taking into account the constraints from electroweak precision measurements, Higgs coupling strength measurements, and unitarity and perturbativity bounds, we identify an interesting region of parameter space leading to enhanced Yukawa couplings as well as enhanced di-Higgs gluon fusion production at the LHC reach. This effect is visible in both t…

PhysicsParticle physicsLarge Hadron ColliderUnitarity010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyElectroweak interactionYukawa potentialFOS: Physical sciencesGeneral Physics and AstronomyFermion01 natural sciencesGluonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Pair production0103 physical sciencesHiggs bosonHigh Energy Physics::Experiment010306 general physicsPhysical Review Letters
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Unitarized Chiral Perturbation Theory in a finite volume: scalar meson sector

2011

We develop a scheme for the extraction of the properties of the scalar mesons f0(600), f0(980), and a0(980) from lattice QCD data. This scheme is based on a two-channel chiral unitary approach with fully relativistic propagators in a finite volume. In order to discuss the feasibility of finding the mass and width of the scalar resonances, we analyze synthetic lattice data with a fixed error assigned, and show that the framework can be indeed used for an accurate determination of resonance pole positions in the multi-channel scattering.

Nuclear and High Energy PhysicsChiral perturbation theoryeffect [threshold]MesonNuclear TheoryHigh Energy Physics::LatticeFOS: Physical scienceschiral [perturbation theory]f0(980)a0(980)Nuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeLattice (order)relativistic [propagator]unitarityddc:530energy levelsScalar mesonnumerical calculationsMathematical physicsPhysicsFinite volume methodScatteringscalar [resonance]High Energy Physics - Lattice (hep-lat)PropagatorFísicascalar mesonLattice QCDf0(600)boundary conditionpole [resonance]High Energy Physics - Phenomenologyfinite size
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Vector form factor of the pion : A model-independent approach

2003

4 páginas, 2 figuras, 3 tablas.-- Comunicación presentada a la 9ª High-Energy Physics International Conference on Quantum ChromoDynamics (QCD 02) celebrada del 2 al 9 de Julio de 2002 en Montpellier (Francia).-- arXiv:hep-ph/0209224v1

PhysicsNuclear and High Energy PhysicsParticle physicsMuonChiral perturbation theoryUnitarityAnomalous magnetic dipole momentHigh Energy Physics::LatticeNuclear TheoryForm factor (quantum field theory)FOS: Physical sciencesFine-structure constantResonance (particle physics)Atomic and Molecular Physics and OpticsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)PionHigh Energy Physics::ExperimentNuclear ExperimentNuclear Physics B - Proceedings Supplements
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Theoretical study of the Ξ(1620) and Ξ(1690) resonances in Ξc→π+MB decays

2017

Nonleptonic weak decays of ${\mathrm{\ensuremath{\Xi}}}_{c}$ into ${\ensuremath{\pi}}^{+}$ and a meson $(M)$-baryon $(B)$ final state, $MB$, are analyzed from the viewpoint of probing $S=\ensuremath{-}2$ baryon resonances, i.e., $\mathrm{\ensuremath{\Xi}}(1620)$ and $\mathrm{\ensuremath{\Xi}}(1690)$, of which spin-parity and other properties are not well known. We argue that the weak decay of ${\mathrm{\ensuremath{\Xi}}}_{c}$ is dominated by a single quark-line diagram, preferred by the Cabibbo-Kobayashi-Maskawa coefficient, color recombination factor, the diquark correlation, and the kinematical condition. The decay process has an advantage of being free from meson resonances in the ${\ens…

PhysicsParticle physicsUnitarityMeson010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyResonanceState (functional analysis)Lambda01 natural sciencesBaryonDiquark0103 physical sciencesInvariant mass010306 general physicsPhysical Review C
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Unitarity constraints on resonance mixing and the Okubo-Zweig-Iizuka rule

1978

We discuss unitarity constraints on the (complex) mixing angle (δ) between resonances. In particular, when the mixing is small, as when it is forbidden by the Okubo-Zweig-Iizuka (OZI) rule, or some other mechanism, one can derive useful bounds on δ or determine Arg (δ) from the data of allowed decays of the resonances. In the case of f′−f mixing the unitarity bound |δ|≳0.05±0.015 is barely compatible with the experimental f′←ππ rate (if one assumes that it is dominated by f′←f←ππ transition). Furthermore, experimentally Im δ≈0 which together with unitarity gives Re δ=−0.08±0.03, in clear discrepancy with the observed f′←ππ rate. This suggests that the mixing of f′ with higher f-like recurre…

PhysicsParticle physicsUnitarity010308 nuclear & particles physics0103 physical sciencesResonanceSymmetry breaking010306 general physics01 natural sciencesMixing (physics)Il Nuovo Cimento A
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