Search results for "ROWE"

showing 10 items of 842 documents

Beyond the Minimal Standard Model

2011

The GSW theory is a great step forward in our understanding of electroweak interactions because it allows the well-known extremely successful theory of quantized electrodynamics and the theory of the weak CC and NC interactions to be cast into one unified, renormalizable local gauge theory. Renormalizability, in particular, is a very desirable property of the theory because it makes covariant perturbation theory a reasonable and well-defined approximation method for calculating physical quantities beyond the lowest order diagrams. Nevertheless, this model, very likely, is not the corner stone of a final theory of weak and electromagnetic interactions. It contains very many parameters which …

PhysicsTheoretical physicsElectroweak interactionAxial currentCovariant transformationParity (physics)Gauge theoryHeavy neutrinoNeutrinoPhysical quantity
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Electromagnetic Processes and Interactions

2011

The electron, the muon, and their neutrinos are important tools in testing the structure of the fundamental electromagnetic and weak interactions. On the other hand, if these interactions are known, they serve as ideal probes for the internal structure of complex hadronic targets such as nucleons and nuclei. Although electroweak interactions should in fact be discussed as a whole and on the same footing, purely electromagnetic interactions play a distinctive role, for obvious experimental reasons: At low and intermediate energies the effective electromagnetic coupling is larger by many orders of magnitude than the weak couplings, so that electromagnetic processes are measurable to much high…

PhysicsTheoretical physicsMuonOrders of magnitude (time)Electroweak interactionForm factor (quantum field theory)ElectronNeutrinoNucleonDeep inelastic scattering
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Electroweak penguins in isospin-violating Bs decays

2011

¯Bs ! φ π 0 and ¯ Bs ! φ ρ 0 , which are dominated by EW penguins. Our results extend the analysis in [1] and have recently been published in [2]. Here we give a brief overview of the outcome. We show that in presence of a new EW penguin amplitude the two Bs branching ratios can be enhanced by an order of magnitude without violating any constraints from other hadronic B decays. This makes them very interesting modes for LHCb and Super B factories. We perform both a model-independent analysis and a study within realistic New Physics (NP) models such as a modified- Z 0 -penguin scenario, a model with an additional Z 0 boson and the MSSM, including a fit to B ! πK data and the relevant experim…

PhysicsTheoretical physicsParticle physicsAmplitudePhysics beyond the Standard ModelIsospinHadronElectroweak interactionOutcome (probability)Order of magnitudeBosonProceedings of 35th International Conference of High Energy Physics — PoS(ICHEP 2010)
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“The Important Thing is not to Stop Questioning”, Including the Symmetries on Which is Based the Standard Model

2014

New fundamental physical theories can, so far a posteriori, be seen as emerging from existing ones via some kind of deformation. That is the basis for Flato’s “deformation philosophy”, of which the main paradigms are the physics revolutions from the beginning of the twentieth century, quantum mechanics (via deformation quantization) and special relativity. On the basis of these facts we describe two main directions by which symmetries of hadrons (strongly interacting elementary particles) may “emerge” by deforming in some sense (including quantization) the Anti de Sitter symmetry (AdS), itself a deformation of the Poincare group of special relativity. The ultimate goal is to base on fundame…

Physicssymbols.namesakeQuantization (physics)Theoretical physicsClassical mechanicsPoincaré groupElectroweak interactionsymbolsHiggs bosonElementary particleAnti-de Sitter spaceEinsteinNoncommutative geometry
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Calculated solar-neutrino capture rate for a radiochemical 205Tl-based solar-neutrino detector

2020

Radiochemical experiments for low-energy solar-neutrino detection have been making headlines by exploiting the isotopes 37Cl and 71Ga. Such a very low-threshold measurement of this type can also be performed using 205Tl, which has been considered for decades for this purpose. A unique feature of this detector nucleus is the integration in the solar-neutrino flux over 106 of years owing to its long-living daughter 205Pb. In this Rapid Communication, we have calculated for the first time the cross section for the charged-current solar-neutrino scattering off 205Tl. Taking into account the solar-model-predicted neutrino fluxes and the electron-neutrino survival probabilities, a solar-neutrino …

Physics::Instrumentation and Detectorselectroweak interactions in nuclear physicsAstrophysics::High Energy Astrophysical Phenomenasolar neutrinosPhysics::Space PhysicsneutriinotAstrophysics::Solar and Stellar AstrophysicsHigh Energy Physics::Experimenthiukkasfysiikkaydinfysiikkanuclear structure and decaysnucleus-neutrino interactions
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The Ratio R of hadronic and electronic Z widths and the strong coupling constant alpha-s

1994

Abstract We review the relation between the ratio of hadronic and electronic Z widths, R = Γ( Z → q q )/Γ( Z → e + e − ) and the strong coupling constant at the Z mass, αs. The theoretical uncertainty of αs derived from R is estimated to be Δα s = ±0.002 (electroweak) ± 0.002 (QCD) −0.003 +0.004 (m top , m Higgs ) .

Quantum chromodynamicsCoupling constantPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::PhenomenologyHadronElectroweak interactionWidth ratiolcsh:QC1-999Nuclear physicsHiggs bosonStrong couplingHigh Energy Physics::ExperimentAstrophysics::Earth and Planetary Astrophysicslcsh:PhysicsParticle Physics - Phenomenology
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and the electroweak penguin contribution

2003

Abstract Our dispersive sum rule calculation of the electroweak penguin contribution to ϵ′ ϵ is reviewed. A more recent analysis based on the finite-energy sum rule approach is described. Finally, a new determination of the electroweak penguin contribution to ϵ′ ϵ is presented.

Quantum chromodynamicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::PhenomenologyElectroweak interactionAtomic and Molecular Physics and OpticsStandard ModelCombinatoricsGrand Unified TheoryHigh Energy Physics::ExperimentPerturbation theory (quantum mechanics)Sum rule in quantum mechanicsGauge theoryOperator product expansionMathematicsNuclear Physics B - Proceedings Supplements
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W+W−Production at Hadron Colliders in Next to Next to Leading Order QCD

2014

Charged gauge boson pair production at the Large Hadron Collider allows detailed probes of the fundamental structure of electroweak interactions. We present precise theoretical predictions for on-shell W+ W- production that include, for the first time, QCD effects up to next to next to leading order in perturbation theory. As compared to next to leading order, the inclusive W+ W- cross section is enhanced by 9% at 7 TeV and 12% at 14 TeV. The residual perturbative uncertainty is at the 3% level. The severe contamination of the W+ W- cross section due to top-quark resonances is discussed in detail. Comparing different definitions of top-free W+ W- production in the four and five flavor numbe…

Quantum chromodynamicsPhysicsGauge bosonParticle physicsLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyHadronElectroweak interactionGeneral Physics and Astronomy7. Clean energy01 natural sciencesCross section (physics)Pair production0103 physical sciencesHigh Energy Physics::ExperimentPerturbation theory (quantum mechanics)010306 general physicsPhysical Review Letters
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Exclusive radiative decays of W and Z bosons in QCD factorization

2015

We present a detailed theoretical analysis of very rare, exclusive hadronic decays of the electroweak gauge bosons V=W, Z from first principles of QCD. Our main focus is on the radiative decays V->M+gamma, in which M is a pseudoscalar or vector meson. At leading order in an expansion in powers of Lambda_{QCD}/m_V the decay amplitudes can be factorized into convolutions of calculable hard-scattering coefficients with the leading-twist light-cone distribution amplitude of the meson M. Power corrections to the decay rates arise first at order (Lambda_{QCD}/m_V)^2. They can be estimated in terms of higher-twist distribution amplitudes and are predicted to be tiny. We include one-loop O(alpha…

Quantum chromodynamicsPhysicsGauge bosonParticle physicsNuclear and High Energy PhysicsMeson010308 nuclear & particles physicsHigh Energy Physics::LatticeElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciences01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)W and Z bosons0103 physical sciencesHigh Energy Physics::ExperimentVector mesonResummation010306 general physicsLeptonJournal of High Energy Physics
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Precision physics with inclusive QCD processes

2021

The inclusive production of hadrons through electroweak currents can be rigorously analysed with short-distance theoretical tools. The associated observables are insensitive to the involved infrared behaviour of the strong interaction, allowing for very precise tests of Quantum Chromodynamics. The theoretical predictions for $\sigma(e^+e^-\to\mathrm{hadrons})$ and the hadronic decay widths of the $\tau$ lepton and the $Z$, $W$ and Higgs bosons have reached an impressive accuracy of $\mathcal{O}(\alpha_s^4)$. Precise experimental measurements of the $Z$ and $\tau$ hadronic widths have made possible the accurate determination of the strong coupling at two very different energy scales, providi…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsElectroweak interactionStrong interactionHigh Energy Physics::PhenomenologyFOS: Physical sciences01 natural sciencesAsymptotic freedomHigh Energy Physics - ExperimentStandard ModelHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHiggs bosonHigh Energy Physics::Experiment010306 general physicsLeptonBoson
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