0000000000053044

AUTHOR

I. Rosell

showing 5 related works from this author

Bottom-up approach within the electroweak effective theory: Constraining heavy resonances

2020

The LHC has confirmed the existence of a mass gap between the known particles and possible new states. Effective field theory is then the appropriate tool to search for low-energy signals of physics beyond the Standard Model. We adopt the general formalism of the electroweak effective theory, with a non-linear realization of the electroweak symmetry breaking, where the Higgs is a singlet with independent couplings. At higher energies we consider a generic resonance Lagrangian which follows the above-mentioned non-linear realization and couples the light particles to bosonic heavy resonances with $J^P=0^\pm$ and $J^P=1^\pm$. Integrating out the resonances and assuming a proper short-distance…

Particle physicsPhotonPhysics beyond the Standard ModelFOS: Physical sciencesMateria - Propiedades.01 natural sciencesColisiones (Física nuclear)Computer Science::Digital LibrariesHigh Energy Physics - Phenomenology (hep-ph)Collisions (Nuclear physics)0103 physical sciencesEffective field theoryPartículas (Física nuclear)Symmetry breakingElectromagnetismo010306 general physicsParticles (Nuclear physics)PhysicsMatter - Properties.010308 nuclear & particles physicsElectroweak interactionHigh Energy Physics::PhenomenologyResonanceHigh Energy Physics - PhenomenologyHiggs bosonMass gapPhysical Review
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One-loop Renormalization of Resonance Chiral Theory with Scalar and Pseudoscalar Resonances

2005

The divergent part of the generating functional of the Resonance Chiral Theory is evaluated up to one loop when one multiplet of scalar an pseudoscalar resonances are included and interaction terms which couple up to two resonances are considered. Hence we obtain the renormalization of the couplings of the initial Lagrangian and, moreover, the complete list of operators that make this theory finite, at this order.

PhysicsNuclear and High Energy PhysicsHigh Energy Physics::LatticeScalar (mathematics)High Energy Physics::PhenomenologyFOS: Physical sciencesResonanceAtomic and Molecular Physics and OpticsRenormalizationPseudoscalarsymbols.namesakeHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)symbolsMultipletLagrangianMathematical physics
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Quantum loops in the Resonance Chiral Theory: improving the vector form factor

2006

Quantum loops in the Resonance Chiral Theory are needed to improve the implementation of non-perturbative QCD. Furthermore, the one-loop computations can predict chiral low-energy couplings at next-to-leading order, a very appealing task. We present a first calculation of the vector form factor of the pion at subleading order in the 1/N_C expansion. From the analysis of the result at large energies we justify the requirement of considering short-distance constraints from form factors with resonances in the final state. The long-distance limit of our results allows to get a next-to-leading order estimate of \ell_6.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsComputationHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyForm factor (quantum field theory)ResonanceOrder (ring theory)FOS: Physical sciencesAtomic and Molecular Physics and OpticsHigh Energy Physics - PhenomenologyPionHigh Energy Physics - Phenomenology (hep-ph)Limit (mathematics)Quantum
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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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Towards a determination of the chiral couplings at NLO in 1/N-C: L-8(r)(μ) and C-38(r)(μ)

2007

14 pages.-- ISI Article Identifier: 000244120200039.-- ArXiv pre-print available at: http://arxiv.org/abs/hep-ph/0610290

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryHigh Energy Physics::LatticeScalar (mathematics)ResonanceOrder (ring theory)FísicaFOS: Physical sciences1/N ExpansionRenormalizationPseudoscalarHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Quantum Chromodynamics (QCD)High Energy Physics::ExperimentPion decay constantChiral lagrangians
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