Search results for "normalization"

showing 10 items of 632 documents

Precision Mass Measurements of Cr58–63 : Nuclear Collectivity Towards the N=40 Island of Inversion

2018

The neutron-rich isotopes $^{58-63}$Cr were produced for the first time at the ISOLDE facility and their masses were measured with the ISOLTRAP spectrometer. The new values are up to 300 times more precise than those in the literature and indicate significantly different nuclear structure from the new mass-surface trend. A gradual onset of deformation is found in this proton and neutron mid-shell region, which is a gateway to the second island of inversion around \emph{N}=40. In addition to comparisons with density-functional theory and large-scale shell-model calculations, we present predictions from the valence-space formulation of the \emph{ab initio} in-medium similarity renormalization…

PhysicsProtonIsotope010308 nuclear & particles physicsIsland of inversionNuclear TheoryAb initioNuclear structureGeneral Physics and AstronomyRenormalization group01 natural sciences7. Clean energyISOLTRAPNuclear physics0103 physical sciencesPhysics::Atomic and Molecular ClustersNeutronNuclear Experiment010306 general physicsPhysical Review Letters
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Infinite projected entangled-pair state algorithm for ruby and triangle-honeycomb lattices

2018

The infinite Projected Entangled-Pair State (iPEPS) algorithm is one of the most efficient techniques for studying the ground-state properties of two-dimensional quantum lattice Hamiltonians in the thermodynamic limit. Here, we show how the algorithm can be adapted to explore nearest-neighbor local Hamiltonians on the ruby and triangle-honeycomb lattices, using the Corner Transfer Matrix (CTM) renormalization group for 2D tensor network contraction. Additionally, we show how the CTM method can be used to calculate the ground state fidelity per lattice site and the boundary density operator and entanglement entropy (EE) on an infinite cylinder. As a benchmark, we apply the iPEPS method to th…

PhysicsQuantum PhysicsStrongly Correlated Electrons (cond-mat.str-el)FOS: Physical sciences02 engineering and technologyQuantum entanglementRenormalization group021001 nanoscience & nanotechnology01 natural sciencesTransfer matrixCondensed Matter - Strongly Correlated ElectronsLattice (order)0103 physical sciencesThermodynamic limitQuantum Physics (quant-ph)010306 general physics0210 nano-technologyAnisotropyAlgorithmQuantumPhase diagramPhysical Review B
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Improved description of the -scattering phenomenology at low energies in covariant baryon chiral perturbation theory

2013

Abstract We present a novel analysis of the π N scattering amplitude in covariant baryon chiral perturbation theory up to O ( p 3 ) within the extended-on-mass-shell renormalization scheme and including the Δ ( 1232 ) explicitly in the δ -counting. We take the hadronic phase shifts provided by partial wave analyses as basic experimental information to fix the low-energy constants. Subsequently, we study in detail the various observables and low-energy theorems related to the π N scattering amplitude. In particular, we discuss the results and chiral expansion of the phase shifts, the threshold coefficients, the Goldberger–Treiman relation, the pion–nucleon sigma term and the extrapolation on…

PhysicsQuantum chromodynamicsChiral perturbation theoryUnitarity010308 nuclear & particles physicsScatteringPartial wave analysisNuclear TheoryGeneral Physics and Astronomy01 natural sciencesBaryonRenormalizationScattering amplitudeQuantum electrodynamicsQuantum mechanics0103 physical sciences010306 general physicsAnnals of Physics
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Three-loop relation of quark $$\overline {MS} $$ and pole masses

1990

We calculate, exactly, the next-to-leading correction to the relation between the $$\overline {MS} $$ quark mass, $$\bar m$$ , and the scheme-independent pole mass,M, and obtain $$\begin{gathered} \frac{M}{{\bar m(M)}} \approx 1 + \frac{4}{3}\frac{{\bar \alpha _s (M)}}{\pi } + \left[ {16.11 - 1.04\sum\limits_{i = 1}^{N_F - 1} {(1 - M_i /M)} } \right] \hfill \\ \cdot \left( {\frac{{\bar \alpha _s (M)}}{\pi }} \right)^2 + 0(\bar \alpha _s^3 (M)), \hfill \\ \end{gathered} $$ as an accurate approximation forN F−1 light quarks of massesM i <M. Combining this new result with known three-loop results for $$\overline {MS} $$ coupling constant and mass renormalization, we relate the pole mass to the…

PhysicsQuantum chromodynamicsCoupling constantQuarkParticle physicsPhysics and Astronomy (miscellaneous)High Energy Physics::PhenomenologyPropagatorElementary particleLoop (topology)RenormalizationHigh Energy Physics::ExperimentEngineering (miscellaneous)Bar (unit)Zeitschrift für Physik C Particles and Fields
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QCD corrections to inclusive ΔS = 1, 2 transitions at the next-to-leading order

1994

24 páginas, 3 figuras, 2 tablas.-- arXiv:hep-ph/9402363v1

PhysicsQuantum chromodynamicsDeltaNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFísicaApproxRenormalizationHigh Energy Physics - PhenomenologyOperator (computer programming)High Energy Physics::ExperimentParticle Physics - TheoryLarge sizeNuclear Physics B
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The massive analytic invariant charge in QCD

2004

The low energy behavior of a recently proposed model for the massive analytic running coupling of QCD is studied. This running coupling has no unphysical singularities, and in the absence of masses displays infrared enhancement. The inclusion of the effects due to the mass of the lightest hadron is accomplished by employing the dispersion relation for the Adler D function. The presence of the nonvanishing pion mass tames the aforementioned enhancement, giving rise to a finite value for the running coupling at the origin. In addition, the effective charge acquires a "plateau-like" behavior in the low energy region of the timelike domain. This plateau is found to be in agreement with a number…

PhysicsQuantum chromodynamicsHigh Energy Physics - TheoryNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesRenormalization groupEffective nuclear chargeHigh Energy Physics - PhenomenologyPionHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)Invariant massSymmetry breakingChiral symmetry breakingLepton
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Chiral perturbation theory: Introduction and recent results in the one-nucleon sector

2009

We provide an introduction to the basic concepts of chiral perturbation theory and discuss some recent developments in the manifestly Lorentz-invariant formulation of the one-nucleon sector.

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsChiral perturbation theoryNuclear TheoryMesonSpontaneous symmetry breakingHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyFOS: Physical sciencesNuclear Theory (nucl-th)RenormalizationHigh Energy Physics - PhenomenologyTheoretical physicsHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Goldstone bosonBibliographyNucleonProgress in Particle and Nuclear Physics
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QCD condensates from tau-decay data: A functional approach

2004

We study a functional method to extract the V − A condensate of dimension 6 from a comparison of τ -decay data with the asymptotic space-like QCD prediction. Our result is in agreement within errors with that from conventional analyses based on finite energy sum rules.

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsFunctional approachFOS: Physical sciencesPerturbation (Mathematics)Mathematical analysisRenormalization (Physics)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Dimension (vector space)Quantum mechanics[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Quantum chromodynamics -- Mathematical modelsSum rule in quantum mechanicsEnergy (signal processing)
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Nonperturbative comparison of QCD effective charges

2009

We study the non-perturbative behavior of two versions of the QCD effective charge, one obtained from the pinch technique gluon self-energy, and one from the ghost-gluon vertex. Despite their distinct theoretical origin, due to a fundamental identity relating various of the ingredients appearing in their respective definitions, the two effective charges are almost identical in the entire range of physical momenta, and coincide exactly in the deep infrared, where they freeze at a common finite value. Specifically, the dressing function of the ghost propagator is related to the two form factors in the Lorentz decomposition of a certain Green's function, appearing in a variety of field-theoret…

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsLorentz transformationHigh Energy Physics::LatticeFOS: Physical sciencesPropagatorFísicaLorentz covarianceEffective nuclear chargeRenormalizationsymbols.namesakeTheoretical physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Classical mechanicsSelf-energysymbolsQuantum field theory
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BK-parameter fromNf=2twisted mass lattice QCD

2011

We present an unquenched Nf=2 lattice computation of the B K parameter which controls K0-K0 oscillations. A partially quenched setup is employed with two maximally twisted dynamical (sea) light Wi ...

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::LatticeLattice field theoryHadronElementary particleLattice QCD01 natural sciencesRenormalizationLattice gauge theoryLattice (order)0103 physical sciences010306 general physicsPhysical Review D
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