Search results for "Reno"

showing 10 items of 1031 documents

The Tensor Networks Anthology: Simulation techniques for many-body quantum lattice systems

2019

We present a compendium of numerical simulation techniques, based on tensor network methods, aiming to address problems of many-body quantum mechanics on a classical computer. The core setting of this anthology are lattice problems in low spatial dimension at finite size, a physical scenario where tensor network methods, both Density Matrix Renormalization Group and beyond, have long proven to be winning strategies. Here we explore in detail the numerical frameworks and methods employed to deal with low-dimension physical setups, from a computational physics perspective. We focus on symmetries and closed-system simulations in arbitrary boundary conditions, while discussing the numerical dat…

Quantum PhysicsComputer simulationComputer scienceLattice problemDensity matrix renormalization groupPhysicsQC1-999FOS: Physical sciencesData structure01 natural sciences010305 fluids & plasmasAlgebra0103 physical sciencesLinear algebraBoundary value problemQuantum Physics (quant-ph)010306 general physicsProgrammerQuantum
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Resonance saturation of the chiral couplings at next-to-leading order in 1/N-C

2009

9 páginas, 3 figuras.-- ISI article identifier:000266408300099.-- ArXiv pre-print avaible at:http://arxiv.org/abs/0903.2440

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsChiral perturbation theoryHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyOrder (ring theory)ResonanceRenormalizationQuantum mechanicsGoldstone bosonSaturation (graph theory)Perturbation theory (quantum mechanics)Mathematical physics
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One-loop renormalization of Resonance Chiral Theory: scalar and pseudoscalar resonances

2005

We consider the Resonance Chiral Theory with one multiplet of scalar and pseudoscalar resonances, up to bilinear couplings in the resonance fields, and evaluate its beta-function at one-loop with the use of the background field method. Thus we also provide the full set of operators that renormalize the theory at one loop and render it finite.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsChiral perturbation theoryScalar field theoryBackground field methodHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyScalar (mathematics)FOS: Physical sciencesRenormalizationPseudoscalarHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Quantum electrodynamicsMultipletMathematical physicsJournal of High Energy Physics
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QCD matching conditions at thresholds

1993

The use of MS-like renormalization schemes in QCD requires an implementation of nontrivial matching conditions across thresholds, a fact often overlooked in the literature. We shortly review the use of these matching conditions in QCD and check explicitly that the prediction for $\alpha_s(M_Z)$, obtained by running the strong coupling constant from the $M_\tau$ scale, does not substantially depend on the exact value of the matching point chosen in crossing the $b$-quark threshold when the appropriate matching conditions are taken into account.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsMatching (statistics)Particle physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaScale (descriptive set theory)RenormalizationHigh Energy Physics - PhenomenologyAlpha (programming language)High Energy Physics - Phenomenology (hep-ph)Strong couplingPoint (geometry)High Energy Physics::ExperimentStatistical physicsConstant (mathematics)Particle Physics - Theory
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Perturbative chiral violations for domain-wall QCD with improved gauge actions

2006

We investigate, in the framework of perturbation theory at finite $N_s$, the effectiveness of improved gauge actions in suppressing the chiral violations of domain-wall fermions. Our calculations show substantial reductions of the residual mass when it is compared at the same value of the gauge coupling, the largest suppression being obtained when the DBW2 action is used. Similar effects can also be observed for a power-divergent mixing coefficient which is chirally suppressed. No significant reduction instead can be seen in the case of the difference between the vector and axial-vector renormalization constants when improved gauge actions are used in place of the plaquette action. We also …

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)FOS: Physical sciencesFermionGauge (firearms)01 natural sciencesRenormalizationDomain wall (string theory)High Energy Physics - LatticeLattice gauge theory0103 physical sciencesPerturbation theory (quantum mechanics)010306 general physicsMixing (physics)
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Measurement of the strong coupling constant alfa_s from global event-shape variables of hadronic Z decays

1991

Abstract An analysis of global event-shape variables has been carried out for the reaction e+e−→Z0→hadrons to measure the strong coupling constant αs. This study is based on 52 720 hadronic events obtained in 1989/90 with the ALEPH detector at the LEP collider at energies near the peak of the Z-resonance. In order to determine αs, second order QCD predictions modified by effects of perturbative higher orders and hadronization were fitted to the experimental distributions of event-shape variables. From a detailed analysis of the theoretical uncertainties we find that this approach is best justified for the differential two-jet rate, from which we obtain αs(MZ2) = 0.121 ± 0.002(stat.)±0.003(s…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsElectron–positron annihilationHadronMeasure (mathematics)Hadronizationlaw.inventionNuclear physicsRenormalizationlawHigh Energy Physics::ExperimentColliderConstant (mathematics)Particle Physics - Experiment
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Form-factors and current correlators: chiral couplingsL10r(μ) andC87r(μ) at NLO in 1/NC

2008

Using the resonance chiral theory Lagrangian, we perform a calculation of the vector and axial-vector two-point functions at the next-to-leading order (NLO) in the 1/N-C expansion. We have analyzed these correlators within the single-resonance approximation and have also investigated the corrections induced by a second multiplet of vector and axial-vector resonance states. Imposing the correct QCD short-distance constraints, one determines the difference of the two correlators Pi(t) equivalent to Pi(VV)(t)-Pi(AA)(t) in terms of the pion decay constant and resonance masses. Its low momentum expansion fixes then the low-energy chiral couplings L 1 0 and C 8 7 at NLO, keeping full control of t…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsFísicaOrder (ring theory)Resonance (particle physics)RenormalizationMomentumPiHigh Energy Physics::ExperimentPion decay constantMultipletJournal of High Energy Physics
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The vector form factor at the next-to-leading order in 1/N(C): chiral couplings L9(mu) and C88(mu) - C90(mu)

2010

24 páginas, 3 figuras, 2 tablas.-- arXiv:1011.5771v1.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeForm factor (quantum field theory)Order (ring theory)ResonanceFOS: Physical sciencesFísica1/N ExpansionQCDRenormalizationMomentumHigh Energy Physics - PhenomenologyPionHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentPion decay constantNuclear ExperimentChiral lagrangians
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Origin of the Large Perturbative Corrections to Higgs Production at Hadron Colliders

2008

The very large K-factor for Higgs-boson production at hadron colliders is shown to result from enhanced perturbative corrections of the form (C_A\pi\alpha_s)^n, which arise in the analytic continuation of the gluon form factor to time-like momentum transfer. These terms are resummed to all orders in perturbation theory using the renormalization group. After the resummation, the K-factor for the production of a light Higgs boson at the LHC is reduced to a value close to 1.3.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyForm factor (quantum field theory)Drell–Yan processFOS: Physical sciencesGluonRenormalizationHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Higgs bosonProduction (computer science)High Energy Physics::ExperimentResummation
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Charmonium properties in hot quenched lattice QCD

2012

We study the properties of charmonium states at finite temperature in quenched QCD on large and fine isotropic lattices. We perform a detailed analysis of charmonium correlation and spectral functions both below and above $T_c$. Our analysis suggests that both S wave states ($J/\psi$ and $\eta_c$) and P wave states ($\chi_{c0}$ and $\chi_{c1}$) disappear already at about $1.5 T_c$. The charm diffusion coefficient is estimated through the Kubo formula and found to be compatible with zero below $T_c$ and approximately $1/\pi T$ at $1.5 T_c\lesssim T\lesssim 3 T_c$.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsSpectral representationNuclear TheoryHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyFOS: Physical sciencesLattice QCDRenormalizationNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeKubo formulaLattice (order)Condensed Matter::SuperconductivityQuark–gluon plasmaCondensed Matter::Strongly Correlated ElectronsHigh Energy Physics::ExperimentNuclear theory
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