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showing 10 items of 2571 documents

Electromagnetism in nonleptonic weak interactions

2000

16 páginas, 1 figura.-- PACS: 11.30.Rd; 13.25.Es; 13.40.Ks.-- arXiv:hep-ph/0006172v2

PhysicsNuclear and High Energy PhysicsParticle physicsRenormalizationPhotonIsospin violationOrder (ring theory)FOS: Physical sciencesFísicaRenormalizationsymbols.namesakeTheoretical physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)ElectromagnetismEffective lagrangiansChiral perturbation theorysymbolsEffective field theoryNonleptonic weak interactionsLagrangian
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Consistency of the triplet seesaw model revisited

2015

14 pages.- 5 figures

PhysicsNuclear and High Energy PhysicsParticle physicsScalar field theoryScalar (mathematics)FísicaFOS: Physical sciencesScalar potentialRenormalization-group equationsScalar bosonGeneral Relativity and Quantum CosmologyHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometryQuantum-field theoryHiggs bosonQuantum field theoryScalar field
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Soft masses in supersymmetric SO(10) GUTs with low intermediate scales

2011

The specific shape of the squark, slepton and gaugino mass spectra, if measured with sufficient accuracy, can provide invaluable information not only about the dynamics underpinning their origin at some very high scale such as the unification scale ${M}_{G}$, but also about the intermediate scale physics encountered throughout their renormalization group equations evolution down to the energy scale accessible for the LHC. In this work, we study general features of the TeV scale soft supersymmetry breaking parameters stemming from a generic mSugra configuration within certain classes of supersymmetry $SO(10)$ GUTs with different intermediate symmetries below ${M}_{G}$. We show that particula…

PhysicsNuclear and High Energy PhysicsParticle physicsScale (ratio)010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyGauginoFísicaSupersymmetryRenormalization group01 natural sciencesSupersymmetry breakingSeesaw molecular geometry0103 physical sciencesHomogeneous spaceHigh Energy Physics::ExperimentSO(10)010306 general physicsPhysical Review D
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Enhanced lepton flavor violation in the supersymmetric inverse seesaw model

2004

We discuss a supersymmetric inverse seesaw model in which lepton flavour violating decays can be enhanced either by flavour violating slepton contributions or by the non-unitarity of the charged current mixing matrix. As an example we calculate Br(mu -> e gamma) taking into account both heavy lepton exchange as well as supersymmetric diagrams in a minimal supergravity framework. We find that the for the same parameters the rate can be enhanced with respect to seesaw model expectations, with or without supersymmetry.

PhysicsNuclear and High Energy PhysicsParticle physicsSolar neutrinoSupergravityHigh Energy Physics::PhenomenologyFlavourFOS: Physical sciencesFísicaSupersymmetryRenormalization groupHigh Energy Physics - PhenomenologyHigh Energy Physics::TheoryHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometryHigh Energy Physics::ExperimentCharged currentLeptonPhysical Review D
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One-loop effective lagrangian for an extension of the standard model with a heavy charged scalar singlet

1994

We study several problems related to the construction and the use of effective Lagrangians by considering an extension of the standard model that includes a heavy scalar singlet coupled to the leptonic doublet. Starting from the full renormalizable model, we build an effective field theory by integrating out the heavy scalar. A local effective Lagrangian (up to operators of dimension six) is obtained by expanding the one-loop effective action in inverse powers of the heavy mass. This is done by matching some Green functions calculated with both the full and the effective theories. Using this simple example we study the renormalization of effective Lagrangians in general and discuss how they…

PhysicsNuclear and High Energy PhysicsParticle physicsSpontaneous symmetry breakingPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyScalar (mathematics)Partícules (Física nuclear)RenormalizationStandard Model (mathematical formulation)Theoretical physicsEffective field theoryEffective actionPhenomenology (particle physics)Nuclear Physics B
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Minimal supergravity radiative effects on the tri-bimaximal neutrino mixing pattern

2007

7 pages, 3 figures.-- PACS nrs.: 14.60.Pq, 12.60.Jv.-- ISI Article Identifier: 000245333000012.-- ArXiv pre-print available at: http://arxiv.org/abs/hep-ph/0606082

PhysicsNuclear and High Energy PhysicsParticle physicsSupergravityHigh Energy Physics::PhenomenologyNumber nonconservation[PACS] Supersymmetric unified modelsFOS: Physical sciencesFísicaWeinberg angleSupersymmetry[PACS] Neutrino mass and mixingMass operator renormalizationSupersymmetry breakingHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Radiative transferSymmetry breakingNeutrinoRight symmetry-breakingMixing (physics)
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Unification of gauge couplings and the tau-neutrino mass in supergravity without R parity

1999

Minimal R-parity violating supergravity predicts a value for $alpha_s(M_Z)$ smaller than in the case with conserved R-parity, and therefore closer to the experimental world average. We show that the R-parity violating effect on the $alpha_s$ prediction comes from the larger two-loop b-quark Yukawa contribution to the renormalization group evolution of the gauge couplings which characterizes R-parity violating supergravity. The effect is correlated to the tau neutrino mass and is sensitive to the initial conditions on the soft supersymmetry breaking parameters at the unification scale. We show how a few percent effect on $alpha_s(M_Z)$ may naturally occur even with tau neutrino masses as sma…

PhysicsNuclear and High Energy PhysicsParticle physicsSupergravityHigh Energy Physics::PhenomenologyYukawa potentialFOS: Physical sciencesFísicaGauge (firearms)Renormalization groupSupersymmetry breakingHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)R-parityTau neutrinoHigh Energy Physics::ExperimentNeutrino oscillation
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Gluon spectrum in the glasma from JIMWLK evolution

2011

The JIMWLK equation with a "daughter dipole" running coupling is solved numerically starting from an initial condition given by the McLerran-Venugopalan model. The resulting Wilson line configurations are then used to compute the spectrum of gluons comprising the glasma inital state of a high energy heavy ion collision. The development of a geometrical scaling region makes the spectrum of produced gluons harder. Thus the ratio of the mean gluon transverse momentum to the saturation scale grows with energy. Also the total gluon multiplicity increases with energy slightly faster than the saturation scale squared.

PhysicsNuclear and High Energy PhysicsParticle physicsWilson loopta114Nuclear Theory010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesYang–Mills existence and mass gapRenormalization group01 natural sciencesGluonNuclear Theory (nucl-th)High Energy Physics - PhenomenologyDipoleHigh Energy Physics - Phenomenology (hep-ph)Quantum electrodynamics0103 physical sciencesInitial value problemBoundary value problem010306 general physicsNuclear ExperimentScaling
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Measurement of α from the structure of particle clusters produced in hadronic Z decays

1991

Abstract Using 106 000 hadronic events obtained with the ALEPH detector at LEP at energies close to the Z resonance peak, the strong coupling constant αs is measured by an analysis of energy-energy correlations (EEC) and the global event shape variables thrust, C-parameter and oblateness. It is shown that the theoretical uncertainties can be significantly reduced if the final state particles are first combined in clusters using a minimum scaled invariant mass cut, Ycut, before these variables are computed. The combined result from all shape variables of pre-clustered events is αs(MZ2 = 0.117±0.005 for a renormalization scale μ= 1 2 M Z . For μ values between MZ and the b-quark mass, the res…

PhysicsNuclear and High Energy PhysicsParticle physicsmedia_common.quotation_subjectElectron–positron annihilationHadronAsymmetryResonance (particle physics)RenormalizationNuclear physicsParticleHigh Energy Physics::ExperimentInvariant massEvent (particle physics)Particle Physics - Experimentmedia_commonPhysics Letters B
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Spin-dipole nuclear matrix elements for double beta decays and astro-neutrinos

2014

Spin-dipole (SD) nuclear matrix elements (NMEs) M±(SD2) for unique first forbidden β±2−→0+ ground-state-to-ground-state transitions are studied by using effective microscopic two-nucleon interactions in realistic single-particle model spaces. The observed values of the NMEs Mexp±(SD2) are compared with the values of the single-quasiparticle NMEs Mqp±(SD2) without nucleon spin–isospin (στ) correlation and the QRPA NMEs MQRPA±(SD2) with the στ correlation. The observed SD matrix elements are found to be reduced by the factor k≈0.2 with respect to Mqp±(SD2) and by the factor kNM≈0.5 with respect to MQRPA±(SD2). We then infer that the SD NME is reduced considerably partly by the nucleon στ corr…

PhysicsNuclear and High Energy PhysicsParticle physicsta114Renormalization of the axial-vector weak coupling constantPhysics::Medical PhysicsNuclear Theorycoupling constantdouble beta decayrenormalization of the axial-vector weakDouble beta decayspin-dipole matrix elementNuclear physicsDipoleMatrix (mathematics)Double beta decaySpin-dipole matrix elementBeta (velocity)Neutrinounique forbidden beta decayNuclear ExperimentSpin (physics)NucleonUnique forbidden beta decayPhysics Letters B
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