Search results for "normalization"

showing 10 items of 632 documents

Critical point Higgs inflation in the Palatini formulation

2021

We study Higgs inflation in the Palatini formulation with the renormalisation group improved potential in the case when loop corrections generate a feature similar to an inflection point. Assuming that there is a threshold correction for the Higgs quartic coupling $\lambda$ and the top Yukawa coupling $y_t$, we scan the three-dimensional parameter space formed by the two jumps and the non-minimal coupling $\xi$. The spectral index $n_s$ can take any value in the observationally allowed range. The lower limit for the running is $\alpha_s>-3.5\times10^{-3}$, and $\alpha_s$ can be as large as the observational upper limit. Running of the running is small. The tensor-to-scalar ratio is $2.2\tim…

Nuclear and High Energy PhysicsCosmology and Nongalactic Astrophysics (astro-ph.CO)FOS: Physical sciencesRIEMANNGeneral Relativity and Quantum Cosmology (gr-qc)Parameter spaceINITIAL CONDITIONSkosmologia01 natural sciences114 Physical sciencesGeneral Relativity and Quantum CosmologyEINSTEINCritical point (thermodynamics)0103 physical sciencesRenormalization Grouplcsh:Nuclear and particle physics. Atomic energy. Radioactivityteoreettinen fysiikkaGENERAL-RELATIVITY010306 general physicscosmology of theories beyond the SMDISSIPATIONBosonMathematical physicsInflation (cosmology)Physics010308 nuclear & particles physicsYukawa potentialCONSTRAINTSBOSONGRAVITATIONRenormalization groupAFFINE VARIATIONAL-PRINCIPLESCosmology of Theories beyond the SMInflection pointHiggs bosonSCALARONlcsh:QC770-798renormalization groupAstrophysics - Cosmology and Nongalactic AstrophysicsJournal of High Energy Physics
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Pinning down the strength function for ordinary muon capture on 100Mo

2019

Ordinary muon capture (OMC) on 100Mo is studied both experimentally and theoretically in order to access the weak responses in wide energy and momentum regions. The OMC populates states in 100Nb up to some 50 MeV in excitation energy. For the first time the associated OMC strength function has been computed and compared with the obtained data. The present computations are performed using the Morita-Fujii formalism of OMC by extending the original formalism beyond the leading order. The participant nuclear wave functions are obtained in extended no-core single-particle model space using the spherical version of proton-neutron quasiparticle random-phase approximation (pnQRPA) with two-nucleon…

Nuclear and High Energy PhysicsIsoscalarmuon-capture giant resonanceNuclear Theorydouble beta decaynuclear matrix elementshiukkasfysiikka01 natural sciencesRenormalization0103 physical sciencesordinary muon capture010306 general physicsWave functionNuclear Experimentvalues of weak axial couplingsPhysicsIsovector010308 nuclear & particles physicslcsh:QC1-999Muon captureGiant resonanceQuantum electrodynamicsIsospinQuasiparticleydinfysiikkacapture-rate distributionlcsh:Physics
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Effective field theory after a new-physics discovery

2018

When a new heavy particle is discovered at the LHC or at a future high-energy collider, it will be interesting to study its decays into Standard Model particles using an effective field-theory framework. We point out that the proper effective theory can not be constructed as an expansion in local, higher-dimensional operators; rather, it must be based on non-local operators defined in soft-collinear effective theory (SCET). For the interesting case where the new resonance is a gauge-singlet spin-0 boson, which is the first member of a new sector governed by a mass scale $M$, we show how a consistent scale separation between $M$ and the electroweak scale $v$ is achieved up to next-to-next-to…

Nuclear and High Energy PhysicsParticle physics530 PhysicsPhysics beyond the Standard ModelFOS: Physical sciences10192 Physics Institute01 natural sciencesResonance (particle physics)Standard ModelHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesEffective field theoryRenormalization Grouplcsh:Nuclear and particle physics. Atomic energy. Radioactivity3106 Nuclear and High Energy Physics010306 general physicsBosonPhysics010308 nuclear & particles physicsComputer Science::Information RetrievalHigh Energy Physics::PhenomenologyEffective Field TheoriesRenormalization groupHigh Energy Physics - PhenomenologySoft-collinear effective theoryBeyond Standard Modellcsh:QC770-798ResummationElectroweak scaleJournal of High Energy Physics
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The Hunt for New Physics at the Large Hadron Collider

2010

233 páginas.-- AHEP Group: et al..-- El Pdf del artículo es la versión pre-print: arXiv.1001.2693v1.-- Trabajo presentado al "The International Workshop on Beyond the Standard Model Physics and LHC Signatures (BSM-LHC) celebrado en Boston (USA) del 2 al 4 de junio de 2009.

Nuclear and High Energy PhysicsParticle physicsCold dark matterPhysics::Instrumentation and DetectorsPhysics beyond the Standard ModelFOS: Physical sciencesRANDALL-SUNDRUM MODEL01 natural sciencesHigh Energy Physics - Phenomenology (hep-ph)R-PARITY BREAKING0103 physical sciencesHigh Energy PhysicsANOMALOUS MAGNETIC-MOMENT010306 general physicsParticle Physics - PhenomenologyPhysicsEXPLICIT CP VIOLATIONDARK-MATTER DETECTIONLarge Hadron Collider010308 nuclear & particles physicsPhysicsElectroweak interactionHigh Energy Physics::PhenomenologyFísicaRENORMALIZATION-GROUP EQUATIONSHierarchy problemSupersymmetryAtomic and Molecular Physics and OpticsGRAND UNIFIED THEORIESSUPERSYMMETRIC STANDARD MODELHidden sectorExtra dimensionsHigh Energy Physics - PhenomenologyMINIMAL FLAVOR VIOLATION[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]PhenomenologyHigh Energy Physics::ExperimentHIGGS-BOSON PRODUCTION
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From transition magnetic moments to majorana neutrino masses

2005

It is well known that a majorana mass induces a (small) transition magnetic moment. The converse is also true; in this paper we estimate the loop contribution of transition magnetic moments $[\mu]_{\alpha \beta}$ to the neutrino mass matrix $[m]_{\alpha \beta}$. We show that for hierarchical neutrino masses, the contribution of $[\mu]_{e \tau}$ to $[m]_{e \tau}$ can exceed the experimental value of $[m]_{e \tau}$.

Nuclear and High Energy PhysicsParticle physicsFOS: Physical sciences01 natural sciencesNuclear physicsHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesmental disorders010306 general physicsM-matrixPhysicsMagnetic moment010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaRenormalization groupMass matrixequipment and suppliesLoop (topology)MAJORANAHigh Energy Physics - Phenomenology[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]NeutrinoMass hierarchyhuman activities
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Muon Anomaly from Lepton Vacuum Polarization and The Mellin--Barnes Representation

2008

We evaluate, analytically, a specific class of eighth--order and tenth--order QED contributions to the anomalous magnetic moment of the muon. They are generated by Feynman diagrams involving lowest order vacuum polarization insertions of leptons $l=e,\mu$, and $\tau$. The results are given in the form of analytic expansions in terms of the mass ratios $m_e/m_\mu$ and $m_\mu/m_\tau$. We compute as many terms as required by the error induced by the present experimental uncertainty on the lepton masses. We show how the Mellin--Barnes integral representation of Feynman parametric integrals allows for an easy analytic evaluation of as many terms as wanted in these expansions and how its underlyi…

Nuclear and High Energy PhysicsParticle physicsFOS: Physical sciences01 natural sciencesRenormalizationsymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)Vacuum PolarizationMuon Anomaly0103 physical sciencesFeynman diagramVacuum polarization010306 general physicsMathematical physicsPhysicsMuonMellin-Barnes RepresentationAnomalous magnetic dipole moment010308 nuclear & particles physicsConverse MappingRenormalization groupHigh Energy Physics - PhenomenologyMultidimensional Residues[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]symbolsAnomaly (physics)Lepton
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B parameters of the complete set of matrix elements of delta B = 2 operators from the lattice

2001

We compute on the lattice the ``bag'' parameters of the five (Delta B = 2) operators of the supersymmetric basis, by combining their values determined in full QCD and in the static limit of HQET. The extrapolation of the QCD results from the accessible heavy-light meson masses to the B-meson mass is constrained by the static result. The matching of the corresponding results in HQET and in QCD is for the first time made at NLO accuracy in the MSbar(NDR) renormalization scheme. All results are obtained in the quenched approximation.

Nuclear and High Energy PhysicsParticle physicsMesonHigh Energy Physics::LatticeSTANDARD MODELExtrapolationLattice (group)FOS: Physical sciencesQuenched approximationHigh Energy Physics - ExperimentSettore FIS/04 - Fisica Nucleare e SubnucleareRenormalizationMatrix (mathematics)High Energy Physics - Experiment (hep-ex)High Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Quantum chromodynamicsPhysicsNONPERTURBATIVE RENORMALIZATIONBasis (linear algebra)High Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyFísicaHigh Energy Physics - PhenomenologyQUARK MASSHigh Energy Physics::ExperimentHEAVY QUARKS
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Running of the Charm-Quark Mass from HERA Deep-Inelastic Scattering Data

2017

Physics letters / B 775, 233 - 238 (2017). doi:10.1016/j.physletb.2017.11.002

Nuclear and High Energy PhysicsParticle physicsPhotonHigh Energy Physics::LatticeFOS: Physical sciencesContext (language use)53001 natural sciencesCharm quarkrenormalizationNuclear physicsHigh Energy Physics - Phenomenology (hep-ph)deep inelastic scattering0103 physical sciencesddc:530Charm (quantum number)quantum chromodynamics: perturbation theory010306 general physicsPhysicsQuantum chromodynamics010308 nuclear & particles physicsScatteringPhysicsHigh Energy Physics::Phenomenologyhigher-order: 1charm: productionHERADeep inelastic scatteringlcsh:QC1-999quark: massHigh Energy Physics - PhenomenologyDESY HERA Storscale dependence[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::Experiment[ PHYS.HPHE ] Physics [physics]/High Energy Physics - Phenomenology [hep-ph]charmlcsh:Physics
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Charm and hidden charm scalar mesons in the nuclear medium

2009

We study the renormalization of the properties of low-lying charm and hidden charm scalar mesons in a nuclear medium, concretely of the D-s0(2317) and the theoretical hidden charm state X(3700). We find that for the D-s0(2317), with negligible width at zero density, the width becomes about 100 MeV at normal nuclear-matter density, while in the case of the X(3700) the width becomes as large as 200 MeV. We discuss the origin of this new width and trace it to reactions occurring in the nucleus, while offering a guideline for future experiments testing these changes. We also show how those medium modifications will bring valuable information on the nature of the scalar resonances and the mechan…

Nuclear and High Energy PhysicsParticle physicsTrace (linear algebra)Nuclear TheoryMesonNuclear TheoryScalar (mathematics)FOS: Physical sciencesCHIRAL-SYMMETRY RESTORATIONNuclear Theory (nucl-th)RenormalizationUNITARY APPROACHCharm (quantum number)Nuclear ExperimentNN INTERACTIONPhysicsHEAVY MESONSZero (complex analysis)FísicaLOCAL SYMMETRYMULTIQUARK HADRONSNuclear matterGAUGE BOSONPHI-PHOTOPRODUCTIONHigh Energy Physics::ExperimentPI-PI INTERACTIONNucleonVECTOR-MESONSThe European Physical Journal A
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s-wave pion-nucleus optical potential

2007

We calculate the s-wave part of the pion-nucleus optical potential using a unitarized chiral approach that has been previously used to simultaneously describe pionic hydrogen and deuterium data as well as low energy pi N scattering in the vacuum. This energy dependent model allows for additional isoscalar parts in the potential from multiple rescattering. We consider Pauli blocking and pion polarization in an asymmetric nuclear matter environment. Also, higher order corrections of the pi N amplitude are included. The model can accommodate the repulsion required by phenomenological fits, though the theoretical uncertainties are bigger than previously thought. At the same time, we also find a…

Nuclear and High Energy PhysicsParticle physicsscattering amplitude [pi nucleon]Nuclear Theorymedia_common.quotation_subjectIsoscalarpartial waveNuclear TheoryFOS: Physical sciencesAsymmetryrenormalizationNuclear physicsNuclear Theory (nucl-th)symbols.namesakePionPauli exclusion principlemesic atom [deuterium]unitarityddc:530higher-order [Feynman graph]nuclear reaction [pi nucleus]numerical calculationsNuclear Experimentmedia_commonPhysicschiral [symmetry]UnitarityIsovectorN(1440)FísicaNuclear mattermesic atom [hydrogen]propagator [pi]Scattering amplitudenuclear mattersymbolsoptical [potential]correction [vertex function]
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