Search results for "renormalization group"

showing 10 items of 206 documents

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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State-of-the-art density matrix renormalization group and coupled cluster theory studies of the nitrogen binding curve.

2004

We study the nitrogen binding curve with the density matrix renormalization group (DMRG) and single-reference and multireference coupled cluster (CC) theory. Our DMRG calculations use up to 4000 states and our single-reference CC calculations include up to full connected hextuple excitations. Using the DMRG, we compute an all-electron benchmark nitrogen binding curve, at the polarized, valence double-zeta level (28 basis functions), with an estimated accuracy of 0.03mE_h. We also assess the performance of more approximate DMRG and CC theories across the nitrogen curve. We provide an analysis of the relative strengths and merits of the DMRG and CC theory under different correlation condition…

Numerical linear algebraValence (chemistry)Density matrix renormalization groupGeneral Physics and Astronomychemistry.chemical_elementBasis functioncomputer.software_genreNitrogenCoupled clusterchemistryMatrix algebraQuantum mechanicsCondensed Matter::Strongly Correlated ElectronsPhysical and Theoretical ChemistrycomputerGroup theoryThe Journal of chemical physics
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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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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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