Search results for "Free parameter"

showing 10 items of 49 documents

Loop quantum gravity and Planck-size black hole entropy

2007

The Loop Quantum Gravity (LQG) program is briefly reviewed and one of its main applications, namely the counting of black hole entropy within the framework is considered. In particular, recent results for Planck size black holes are reviewed. These results are consistent with an asymptotic linear relation (that fixes uniquely a free parameter of the theory) and a logarithmic correction with a coefficient equal to -1/2. The account is tailored as an introduction to the subject for non-experts.

PhysicsHistoryLogarithmFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)Loop quantum gravityLinear-quadratic-Gaussian controlGeneral Relativity and Quantum CosmologyComputer Science ApplicationsEducationsymbols.namesakeTheoretical physicsGeneral Relativity and Quantum CosmologysymbolsLinear relationPlanckBlack hole thermodynamicsFree parameter
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A dispersion theoretical approach to the threshold amplitudes of pion photoproduction

1996

We give predictions for the partial wave amplitudes of pion photoproduction near threshold by means of dispersion relations at fixed t. The free parameters of this approach are determined by a fit to experimental data in the energy range 160 MeV $\le E_{\gamma} \le$ 420 MeV. The observables near threshold are found to be rather sensitive to the amplitudes in the resonance region, in particular to the $\Delta$ (1232) and $N^*$ (1440). We obtain a good agreement with the existing threshold data for both charged and neutral pion production. Our predictions also agree well with the results of chiral perturbation theory, except for neutral pion production off the neutron.

PhysicsNuclear and High Energy PhysicsChiral perturbation theoryNuclear TheoryNuclear TheoryFOS: Physical sciencesObservableResonance (particle physics)Nuclear physicsNuclear Theory (nucl-th)AmplitudePionDispersion relationNeutronNuclear ExperimentFree parameter
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Model-independent separation of structure functions over an extended kinematical region

1994

A method for the separation of structure functions in (e, e′ p) experiments is proposed, which is an extension of the traditional Rosenbluth-type techniques of [1,2]. In our approach, we use a very flexible Ansatz to describe the structure functions within an extended kinematical regionG and determine its free parameters with a x2 minimization. The procedure is tested by pseudo data (12C(e, e′p)11Bg.s.) in the quasi-free region.

PhysicsNuclear and High Energy PhysicsMathematical analysisHadronElementary particleMinificationExtension (predicate logic)FermionNucleonFree parameterAnsatzZeitschrift f�r Physik A Hadrons and Nuclei
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The minimal 3+2 neutrino model versus oscillation anomalies

2012

We study the constraints imposed by neutrino oscillation experiments on the minimal extension of the Standard Model that can explain neutrino masses, which requires the addition of just two singlet Weyl fermions. The most general renormalizable couplings of this model imply generically four massive neutrino mass eigenstates while one remains massless: it is therefore a minimal 3+2 model. The possibility to account for the confirmed solar, atmospheric and long-baseline oscillations, together with the LSND/MiniBooNE and reactor anomalies is addressed. We find that the minimal model can fit oscillation data including the anomalies better than the standard $3\nu$ model and similarly to the 3+2 …

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsFOS: Physical sciencesFísica7. Clean energy01 natural sciencesStandard ModelMiniBooNEMassless particleMinimal modelHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometry0103 physical sciencesNeutrino010306 general physicsNeutrino oscillationFree parameter
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CKM matrix and fermion masses in the dualized standard model

1997

A Dualized Standard Model recently proposed affords a natural explanation for the existence of Higgs fields and of exactly 3 generations of fermions, while giving at the same time the observed fermion mass hierarchy together with a tree-level CKM matrix equal to the identity matrix. It further suggests a method for generating from loop corrections the lower generation masses and nondiagonal CKM matrix elements. In this paper, the proposed calculation is carried out to 1-loop. It is found first that with the method suggested one can account readily for the masses of the second generation fermions as a `leakage' from the highest generation. Then, with the Yukawa couplings fixed by fitting the…

PhysicsNuclear and High Energy PhysicsParticle physicsCabibbo–Kobayashi–Maskawa matrixElectroweak interactionHigh Energy Physics::PhenomenologyIdentity matrixYukawa potentialFOS: Physical sciencesFísicaFermionHigh Energy Physics - PhenomenologyStandard Model (mathematical formulation)High Energy Physics - Phenomenology (hep-ph)Higgs bosonFree parameter
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A non-perturbative chiral approach for meson-meson interactions

2000

A non-perturbative method which combines constraints from chiral symmetry breaking and coupled channel unitarity is used to describe meson-meson interactions up to \sqrt{s}\lesssim 1.2 GeV, extending in this way the range of applicability of the information contained in Chiral Perturbation Theory (\chi PT), since this perturbative series is typically restricted to \sqrt{s}\lesssim 500 MeV. The approach uses the O(p^2) and O(p^4) \chiPT Lagrangians. The seven free parameters resulting from the O(p^4) Lagrangian are fitted to the experimental data. The approach makes use of the expansion of T^{-1} instead of the amplitude itself as done in \chiPT. The former expansion is suggested by analogy …

PhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryFísica-Modelos matemáticosSeries (mathematics)MesonUnitarityFísicaFOS: Physical sciencesHigh Energy Physics - PhenomenologyAmplitudeHigh Energy Physics - Phenomenology (hep-ph)Física matemáticaNon-perturbativeChiral symmetry breakingFree parameter
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Radiative pion capture by a nucleon

2000

The differential cross sections for $\pi^- p \to \gamma n$ and $\pi^+ n \to \gamma p$ are computed up to $O(p^3)$ in heavy baryon chiral perturbation theory (HBChPT). The expressions at $O(p)$ and $O(p^2)$ have no free parameters. There are three unknown parameters at $O(p^3)$, low energy constants of the HBChPT Lagrangian, which are determined by fitting to experimental data. Two acceptable fits are obtained, which can be separated by comparing with earlier dispersion relation calculations of the inverse process. Expressions for the multipoles, with emphasis on the p-wave multipoles, are obtained and evaluated at threshold. Generally the results obtained from the best of the two fits are i…

PhysicsNuclear and High Energy PhysicsParticle physicsHeavy baryon chiral perturbation theoryNuclear Theory010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyInverseFOS: Physical sciences01 natural sciencesJNuclear Theory (nucl-th)symbols.namesakeHigh Energy Physics - PhenomenologyPionHigh Energy Physics - Phenomenology (hep-ph)Dispersion relation0103 physical sciencesRadiative transfersymbolsddc:530010306 general physicsNucleonLagrangianFree parameter
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LHC constraints on two-Higgs doublet models

2013

A new Higgs-like boson with mass around 126 GeV has recently been discovered at the LHC. The available data on this new particle is analyzed within the context of two-Higgs doublet models without tree-level flavour-changing neutral currents. Keeping the generic Yukawa structure of the Aligned Two-Higgs Doublet Model framework, we study the implications of the LHC data on the allowed scalar spectrum. We analyze both the CP-violating and CP-conserving cases, and a few particular limits with a reduced number of free parameters, such as the usual models based on discrete Z(2) symmetries.

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderHiggs PhysicsAcceleradors de partículesScalar (mathematics)High Energy Physics::PhenomenologyYukawa potentialFOS: Physical sciencesContext (language use)Partícules (Física nuclear)High Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Beyond Standard ModelHiggs bosonCP violationHigh Energy Physics::ExperimentBosonFree parameter
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The KATRIN sensitivity to the neutrino mass and to right-handed currents in beta decay

2007

The aim of the KArlsruhe TRItium Neutrino experiment KATRIN is the determination of the absolute neutrino mass scale down to 0.2 eV, with essentially smaller model dependence than from cosmology and neutrinoless double beta decay. For this purpose, the integral electron energy spectrum is measured close to the endpoint of molecular tritium beta decay. The endpoint, together with the neutrino mass, should be fitted from the KATRIN data as a free parameter. The right-handed couplings change the electron energy spectrum close to the endpoint, therefore they have some effect also to the precise neutrino mass determination. The statistical calculations show that, using the endpoint as a free par…

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsFOS: Physical sciencesBeta decayCosmologyNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Double beta decayMeasurements of neutrino speedHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationFree parameterKATRIN
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Electroweak Precision Tests of the Standard Model after the Discovery of the Higgs Boson

2019

The global fit of the Standard Model predictions to electroweak precision data, which has been routinely performed in the past decades by several groups, led to the prediction of the top quark and the Higgs boson masses before their respective discoveries. With the measurement of the Higgs boson mass at the Large Hadron Collider (LHC) in 2012 by the ATLAS and CMS collaborations, the last free parameter of the Standard Model of particle physics has been fixed, and the global electroweak fit can be used to test the full internal consistency of the electroweak sector of the Standard Model and constrain models beyond. In this article, we review the current state-of-the-art theoretical calculati…

PhysicsNuclear and High Energy PhysicsTop quarkParticle physicsLarge Hadron Collider010308 nuclear & particles physicshep-exElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical scienceshep-ph01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Internal consistency0103 physical sciencesHiggs bosonHigh Energy Physics::Experiment010306 general physicsParticle Physics - ExperimentFree parameterParticle Physics - Phenomenology
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