Search results for "Renormalization"

showing 10 items of 470 documents

Deep inelastic scattering in the dipole picture at next-to-leading order

2017

We study quantitatively the importance of the recently derived NLO corrections to the DIS structure functions at small x in the dipole formalism. We show that these corrections can be significant and depend on the factorization scheme used to resum large logarithms of energy into renormalization group evolution with the BK equation. This feature is similar to what has recently been observed for single inclusive forward hadron production. Using a factorization scheme consistent with the one recently proposed for the single inclusive cross section, we show that it is possible to obtain meaningful results for the DIS cross sections.

Particle physicsNuclear TheoryHadronFOS: Physical sciencesInelastic scattering01 natural sciences114 Physical sciencesInelastic neutron scatteringNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)Factorizationnuclear physics0103 physical sciencesPerturbative QCD010306 general physicsPhysicsQuasielastic scatteringta114010308 nuclear & particles physicsRenormalization groupDeep inelastic scatteringEVOLUTIONDipoleHigh Energy Physics - PhenomenologyQCD in nuclear reactionsHigh Energy Physics::ExperimentydinfysiikkaPhysical Review D
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Global effective-field-theory analysis of new-physics effects in (semi)leptonic kaon decays

2016

We analyze the decays $K\to\pi\ell\nu$ and $P\to\ell\nu$ ($P=K,\pi$, $\ell=e,\,\mu$) using a low-energy Effective-Field-Theory approach to parametrize New Physics and study the complementarity with baryon $\beta$ decays. We then provide a road map for a global analysis of the experimental data, with all the Wilson coefficients simultaneously, and perform a fit leading to numerical bounds for them and for $V_{us}$. A prominent result of our analysis is a reinterpretation of the well-known $V_{ud}-V_{us}$ diagram as a strong constraint on new physics. Finally, we reinterpret our bounds in terms of the $SU(2)_L\times~U(1)_Y$-invariant operators, provide bounds to the corresponding Wilson coeff…

Particle physicsNuclear and High Energy PhysicsPhysics beyond the Standard ModelFOS: Physical sciences01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesEffective lagrangian[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Effective field theoryComputer Science::Symbolic Computation010306 general physicsParticle Physics - PhenomenologyPhysicsLarge Hadron Collider[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat]010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics - Lattice (hep-lat)Renormalization groupBaryonHigh Energy Physics - Phenomenology[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Journal of High Energy Physics
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Observation of random-field behavior in (CO)1−x(N2)xmixtures physisorbed on graphite

1993

Heat-capacity studies have been carried out on submonolayers of (CO${)}_{1\mathrm{\ensuremath{-}}\mathit{x}}$(${\mathrm{N}}_{2}$${)}_{\mathit{x}}$ mixtures physisorbed on graphite. We find that pure CO undergoes an end-to-end ordering transition at ${\mathit{T}}_{\mathit{c}}$=5.18 K, which is shown to belong to the two-dimensional Ising universality class. In diluting CO with ${\mathrm{N}}_{2}$ the heat-capacity peaks become progressively rounded until the phase transition is completely suppressed at a ${\mathrm{N}}_{2}$ concentration of only x=0.07. The analysis of the data shows that this behavior is in quantitative agreement with predictions of the random-field theory applied to adsorbed…

Phase transitionCrystallographyMaterials scienceRandom fieldSpecific heatGeneral Physics and AstronomyPhysical chemistryIsing modelGraphiteRenormalization groupHeat capacitySolid solutionPhysical Review Letters
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Polymer mixtures in confined geometries: Model systems to explore phase transitions

2005

While binary (A,B) symmetric polymer mixtures ind = 3 dimensions have an unmixing critical point that belongs to the 3d Ising universality class and crosses over to mean field behavior for very long chains, the critical behavior of mixtures confined into thin film geometry falls in the 2d Ising class irrespective of chain length. The critical temperature always scales linearly with chain length, except for strictly two-dimensional chains confined to a plane, for whichT; c ∝N; 5/8 (this unusual exponent describes the fractal contact line between segregated chains in dense melts in two spatial dimensions, d = 2). When the walls of the thin film are not neutral, but preferentially attract one …

Phase transitionwettingMaterials scienceCondensed matter physicsCapillary condensationPolymersGeneral Physics and AstronomyQuímicaRenormalization groupfinite size scalingMean field theoryCritical point (thermodynamics)ExponentIsing modelphase separationMonte Carlo simulationPhase diagram
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Quantum corrections to inflation: the importance of RG-running and choosing the optimal RG-scale

2017

We demonstrate the importance of correctly implementing RG running and choosing the RG scale when calculating quantum corrections to inflaton dynamics. We show that such corrections are negligible for single-field inflation, in the sense of not altering the viable region in the ${n}_{s}\ensuremath{-}r$ plane, when imposing Planck constraints on ${A}_{s}$. Surprisingly, this also applies, in a nontrivial way, for an inflaton coupled to additional spectator degrees of freedom. The result relies on choosing the renormalization scale (pseudo-)optimally, thereby avoiding unphysical large logarithmic corrections to the Friedmann equations and large running of the couplings. We find that the viabl…

Physics beyond the Standard ModelScalar (mathematics)FOS: Physical sciencesAstrophysics::Cosmology and Extragalactic Astrophysics01 natural sciencesClassical limitRenormalizationsymbols.namesakeGeneral Relativity and Quantum Cosmologyquantum correctionsHigh Energy Physics - Phenomenology (hep-ph)Quantum mechanics0103 physical sciences010306 general physicsQuantumMathematical physicsPhysicsta114010308 nuclear & particles physicsFriedmann equationsInflatonRenormalization groupinflatonHigh Energy Physics - Phenomenologysymbols
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Response functions for infinite fermion systems with velocity dependent interactions

1992

Response functions of infinite Fermi systems are studied in the framework of the self-consistent random phase approximation (RPA). Starting from an effective interaction with velocity and density dependence, or equivalently from a local energy density functional, algebraic expressions for the RPA response function are derived. Simple formulae for the energy-weighted and polarizability sum rules are obtained. The method is illustrated by applications to nuclear matter and liquid 3 He. In nuclear matter, it is shown that existing Skyrme interactions give spin-isospin response functions close to those calculated with finite range interactions. The different renormalization of longitudinal and …

Physics010308 nuclear & particles physicsOscillationNuclear TheoryGeneral Physics and AstronomyFermionNuclear matter01 natural sciencesRenormalizationPolarizabilityQuantum electrodynamicsQuantum mechanics0103 physical sciencesCoulomb010306 general physicsRandom phase approximationEnergy functional
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Numerical integration of subtraction terms

2016

Numerical approaches to higher-order calculations often employ subtraction terms, both for the real emission and the virtual corrections. These subtraction terms have to be added back. In this paper we show that at NLO the real subtraction terms, the virtual subtraction terms, the integral representations of the field renormalisation constants and -- in the case of initial-state partons -- the integral representation for the collinear counterterm can be grouped together to give finite integrals, which can be evaluated numerically. This is useful for an extension towards NNLO.

Physics010308 nuclear & particles physicsSubtractionOrder (ring theory)FOS: Physical sciencesField (mathematics)PartonExtension (predicate logic)01 natural sciencesNumerical integrationRenormalizationHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Quantum electrodynamics0103 physical sciencesApplied mathematicsHardware_ARITHMETICANDLOGICSTRUCTURES010306 general physicsRepresentation (mathematics)
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Examining the N=28 shell closure through high-precision mass measurements of Ar46–48

2020

The strength of the $N=28$ magic number in neutron-rich argon isotopes is examined through high-precision mass measurements of $^{46\text{--}48}\mathrm{Ar}$, performed with the ISOLTRAP mass spectrometer at ISOLDE/CERN. The new mass values are up to 90 times more precise than previous measurements. While they suggest the persistence of the $N=28$ shell closure for argon, we show that this conclusion has to be nuanced in light of the wealth of spectroscopic data and theoretical investigations performed with the SDPF-U phenomenological shell model interaction. Our results are also compared with ab initio calculations using the valence space in-medium similarity renormalization group and the s…

PhysicsArgonValence (chemistry)010308 nuclear & particles physicsSHELL modelchemistry.chemical_elementIsotopes of argonRenormalization groupMass spectrometry01 natural sciencesISOLTRAPchemistryAb initio quantum chemistry methods0103 physical sciencesPhysics::Atomic and Molecular ClustersAtomic physics010306 general physicsPhysical Review C
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The neutrino charge radius is a physical observable

2004

We present a method which allows, at least in principle, the direct extraction of the gauge-invariant and process-independent neutrino charge radius (NCR) from experiments. Under special kinematic conditions, the judicious combination of neutrino and anti-neutrino forward differential cross-sections allows the exclusion of all target-dependent contributions, such as gauge-independent box-graphs, not related to the NCR. We show that the remaining contributions contain universal, renormalization group invariant combinations, such as the electroweak effective charge and the running mixing angle, which must be also separated out. By considering the appropriate number of independent experiments …

PhysicsAstrofísicaNuclear and High Energy PhysicsParticle physicsElectroweak interactionFOS: Physical sciencesWeinberg angleObservableRenormalization groupRenormalizationHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Charge radiusNeutrinoLepton
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Analyzing dynamical gluon mass generation

2007

We study the necessary conditions for obtaining infrared finite solutions from the Schwinger-Dyson equation governing the dynamics of the gluon propagator. The equation in question is set up in the Feynman gauge of the background field method, thus capturing a number of desirable features. Most notably, and in contradistinction to the standard formulation, the gluon self-energy is transverse order-by-order in the dressed loop expansion, and separately for gluonic and ghost contributions. Various subtle field-theoretic issues, such as renormalization group invariance and regularization of quadratic divergences, are briefly addressed. The infrared and ultraviolet properties of the obtained so…

PhysicsBackground field methodHigh Energy Physics::LatticeMass generationHigh Energy Physics::PhenomenologyBackground field methodFOS: Physical sciencesPinch techniqueGeneral Physics and AstronomyPropagatorFísicaRenormalization groupHigh Energy Physics - Phenomenologysymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)Gluon propagatorSchwinger-Dyson equationsGluon field strength tensorRegularization (physics)Quantum electrodynamicssymbolsFeynman diagramGluon fieldRunning couplingMathematical physics
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