Search results for "QC770"

showing 10 items of 270 documents

A model calculation of double parton distribution functions of the pion

2018

Two-parton correlations in the pion are investigated in terms of double parton distribution functions. A Poincar\'e covariant Light-Front framework has been adopted. As non perturbative input, the pion wave function obtained within the so-called soft-wall AdS/QCD model has been used. Results show how novel dynamical information on the structure of the pion, not accessible through one-body parton distribution, are encoded in double parton distribution functions.

Particle physicsPhysics and Astronomy (miscellaneous)Distribution (number theory)High Energy Physics::LatticeFOS: Physical scienceslcsh:AstrophysicsParton01 natural sciencesHigh Energy Physics - Phenomenology (hep-ph)Pionlcsh:QB460-4660103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. RadioactivityCovariant transformation010306 general physicsWave functionNuclear ExperimentEngineering (miscellaneous)Quantum chromodynamicsPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyHigh Energy Physics - PhenomenologyDistribution functionlcsh:QC770-798High Energy Physics::ExperimentNon-perturbativeEuropean Physical Journal
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DeepXS: fast approximation of MSSM electroweak cross sections at NLO

2018

We present a deep learning solution to the prediction of particle production cross sections over a complicated, high-dimensional parameter space. We demonstrate the applicability by providing state-of-the-art predictions for the production of charginos and neutralinos at the Large Hadron Collider (LHC) at the next-to-leading order in the phenomenological MSSM-19 and explicitly demonstrate the performance for $pp\to\tilde{\chi}^+_1\tilde{\chi}^-_1,$ $\tilde{\chi}^0_2\tilde{\chi}^0_2$ and $\tilde{\chi}^0_2\tilde{\chi}^\pm_1$ as a proof of concept which will be extended to all SUSY electroweak pairs. We obtain errors that are lower than the uncertainty from scale and parton distribution functi…

Particle physicsPhysics and Astronomy (miscellaneous)FOS: Physical scienceslcsh:AstrophysicsPartonParameter space53001 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)lcsh:QB460-4660103 physical sciencesddc:530lcsh:Nuclear and particle physics. Atomic energy. RadioactivityHigh Energy Physics010306 general physicsEngineering (miscellaneous)Physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyElectroweak interactionOrder (ring theory)SupersymmetryHigh Energy Physics - PhenomenologyDistribution functionlcsh:QC770-798High Energy Physics::ExperimentMonte Carlo integrationProduction (computer science)
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Lorentz-covariant coordinate-space representation of the leading hadronic contribution to the anomalous magnetic moment of the muon

2017

We present a Lorentz-covariant, Euclidean coordinate-space expression for the hadronic vacuum polarisation, the Adler function and the leading hadronic contribution to the anomalous magnetic moment of the muon. The representation offers a lot of flexibility for an implementation in lattice QCD. We expect it to be particularly helpful for the quark-line disconnected contributions.

Particle physicsPhysics and Astronomy (miscellaneous)Lorentz transformationHigh Energy Physics::LatticeHadronFOS: Physical scienceslcsh:Astrophysics01 natural sciencessymbols.namesakeHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesEuclidean geometrylcsh:QB460-466Covariant transformationlcsh:Nuclear and particle physics. Atomic energy. RadioactivityCoordinate space010306 general physicsEngineering (miscellaneous)PhysicsMuonAnomalous magnetic dipole moment010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyLattice QCDHigh Energy Physics - Phenomenologysymbolslcsh:QC770-798High Energy Physics::ExperimentEuropean Physical Journal C
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The Z boson spin observables as messengers of new physics

2017

We demonstrate that the 8 multipole parameters describing the spin state of the $Z$ boson are able to disentangle known $Z$ production mechanisms and signals from new physics at the LHC. They can be extracted from appropriate asymmetries in the angular distribution of lepton pairs from the $Z$ boson decay. The power of this analysis is illustrated by (i) the production of $Z$ boson plus jets; (ii) $Z$ boson plus missing transverse energy; (iii) $W$ and $Z$ bosons originating from the two-body decay of a heavy resonance.

Particle physicsPhysics and Astronomy (miscellaneous)Physics beyond the Standard ModelFOS: Physical scienceslcsh:Astrophysics01 natural sciencesResonance (particle physics)Light Supersymmetric ParticleHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Standard Model Predictionlcsh:QB460-4660103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsEngineering (miscellaneous)Spin-½BosonCondensed Matter::Quantum GasesPhysicsLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyAngular DistributionCharged LeptonObservable3. Good healthHigh Energy Physics - PhenomenologyLarge Hadron Colliderlcsh:QC770-798High Energy Physics::ExperimentMultipole expansionLeptonThe European Physical Journal C
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GeV-scale neutrinos: interactions with mesons and DUNE sensitivity

2021

The simplest extension of the SM to account for the observed neutrino masses and mixings is the addition of at least two singlet fermions (or right-handed neutrinos). If their masses lie at or below the GeV scale, such new fermions would be produced in meson decays. Similarly, provided they are sufficiently heavy, their decay channels may involve mesons in the final state. Although the couplings between mesons and heavy neutrinos have been computed previously, significant discrepancies can be found in the literature. The aim of this paper is to clarify such discrepancies and provide consistent expressions for all relevant effective operators involving mesons with masses up to 2 GeV. Moreove…

Particle physicsPhysics and Astronomy (miscellaneous)Scale (ratio)MesonFOS: Physical scienceslcsh:Astrophysics01 natural sciences7. Clean energyHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)lcsh:QB460-4660103 physical sciencesDark Matterlcsh:Nuclear and particle physics. Atomic energy. RadioactivityNuclear Experiment010306 general physicsEngineering (miscellaneous)Physics010308 nuclear & particles physicsDirac (video compression format)High Energy Physics::PhenomenologyFísicaFermionLeptonsHigh Energy Physics - PhenomenologyMAJORANAlcsh:QC770-798High Energy Physics::ExperimentNeutrinoNeutrino MassEvent (particle physics)Lepton
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The ultraviolet landscape of two-Higgs doublet models

2018

We study the predictions of generic ultraviolet completions of two-Higgs doublet models. We assume that at the matching scale between the two-Higgs doublet model and a ultraviolet complete theory -- which can be anywhere between the TeV and the Planck scale -- arbitrary but perturbative values for the quartic couplings are present. We evaluate the couplings down from the matching scale to the weak scale and study the predictions for the scalar mass spectrum. In particular, we show the importance of radiative corrections which are essential for both an accurate Higgs mass calculation as well as determining the stability of the electroweak vacuum. We study the relation between the mass splitt…

Particle physicsPhysics and Astronomy (miscellaneous)Scale (ratio)Scalar (mathematics)FOS: Physical scienceslcsh:Astrophysics01 natural sciencesStability (probability)High Energy Physics - Phenomenology (hep-ph)Quartic functionlcsh:QB460-4660103 physical sciencesRadiative transferddc:530lcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsEngineering (miscellaneous)Physics010308 nuclear & particles physicsPhysicsElectroweak interactionHigh Energy Physics::PhenomenologyHigh Energy Physics - PhenomenologyMass spectrumHiggs bosonlcsh:QC770-798Regular Article - Theoretical Physics
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Majorana vs pseudo-Dirac neutrinos at the ILC

2019

Neutrino masses could originate in seesaw models testable at colliders, with light mediators and an approximate lepton number symmetry. The minimal model of this type contains two quasi-degenerate Majorana fermions forming a pseudo-Dirac pair. An important question is to what extent future colliders will have sensitivity to the splitting between the Majorana components, since this quantity signals the breaking of lepton number and is connected to the light neutrino masses. We consider the production of these neutral heavy leptons at the ILC, where their displaced decays provide a golden signal: a forward–backward charge asymmetry, which depends crucially on the mass splitting between the tw…

Particle physicsPhysics and Astronomy (miscellaneous)media_common.quotation_subjectFOS: Physical scienceslcsh:Astrophysics01 natural sciences7. Clean energyAsymmetryHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometryDouble beta decay0103 physical scienceslcsh:QB460-466lcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsEngineering (miscellaneous)media_commonPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFermionLepton numberMAJORANAHigh Energy Physics - Phenomenologylcsh:QC770-798High Energy Physics::ExperimentNeutrinoLepton
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Spontaneous baryogenesis in spiral inflation

2019

We examined the possibility of spontaneous baryogenesis driven by the inflaton in the scenario of spiral inflation, and found the parametric dependence of the late-time baryon number asymmetry. As a result, it is shown that, depending on the effective coupling of baryon/lepton number violating operators, it is possible to obtain the right amount of asymmetry even in the presence of a matter-domination era as long as such era is relatively short. In a part of the parameter space, the required expansion rate during inflation is close to the current upper-bound, and hence can be probed in the near future experiments.

Particle physicsPhysics and Astronomy (miscellaneous)media_common.quotation_subjectFOS: Physical scienceslcsh:AstrophysicsAstrophysics::Cosmology and Extragalactic AstrophysicsParameter space01 natural sciencesAsymmetryHigh Energy Physics - Phenomenology (hep-ph)0103 physical scienceslcsh:QB460-466lcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsEngineering (miscellaneous)media_commonInflation (cosmology)Physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyInflatonLepton numberBaryonBaryogenesisHigh Energy Physics - Phenomenologylcsh:QC770-798Baryon numberEuropean Physical Journal C: Particles and Fields
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Cosmology and CPT violating neutrinos

2017

The combination Charge Conjugation-Parity-Time Reversal(CPT) is a fundamental symmetry in our current understanding of nature. As such, testing CPT violation is a strongly motivated path to explore new physics. In this paper we study CPT violation in the neutrino sector, giving for the first time a bound, for a fundamental particle, in the CPT violating particle-antiparticle gravitational mass difference. We argue that cosmology is nowadays the only data sensitive to CPT violation for the neutrino-antineutrino mass splitting and we use the latest data release from Planck combined with the current Baryonic-Acoustic-Oscillation measurement to perform a full cosmological analysis. To show the …

Particle physicsPhysics::General PhysicsPhysics and Astronomy (miscellaneous)Physics beyond the Standard ModelFOS: Physical sciencesElementary particlelcsh:Astrophysics7. Clean energy01 natural sciencesCosmologyGravitationsymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)0103 physical scienceslcsh:QB460-466lcsh:Nuclear and particle physics. Atomic energy. RadioactivityPlanck010306 general physics010303 astronomy & astrophysicsEngineering (miscellaneous)PhysicsHigh Energy Physics::PhenomenologyCharge (physics)Symmetry (physics)High Energy Physics - Phenomenologysymbolslcsh:QC770-798High Energy Physics::ExperimentNeutrino
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Icecube/DeepCore tests for novel explanations of the MiniBooNE anomaly

2019

While the low-energy excess observed at MiniBooNE remains unchallenged, it has become increasingly difficult to reconcile it with the results from other sterile neutrino searches and cosmology. Recently, it has been shown that non-minimal models with new particles in a hidden sector could provide a better fit to the data. As their main ingredients they require a GeV-scale $Z'$, kinetically mixed with the photon, and an unstable heavy neutrino with a mass in the 150 MeV range that mixes with the light neutrinos. In this letter we point out that atmospheric neutrino experiments (and, in particular, IceCube/DeepCore) could probe a significant fraction of the parameter space of such models by l…

Particle physicsSterile neutrinoPhotonPhysics and Astronomy (miscellaneous)FOS: Physical scienceslcsh:AstrophysicsParameter space01 natural sciencesCosmologyHigh Energy Physics - ExperimentMiniBooNEHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)lcsh:QB460-4660103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsEngineering (miscellaneous)Physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyHidden sectorHigh Energy Physics - Phenomenologylcsh:QC770-798High Energy Physics::ExperimentAnomaly (physics)NeutrinoThe European Physical Journal C
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