Search results for " symmetry"

showing 10 items of 701 documents

Maximal Flavour Violation: a Cabibbo mechanism for leptoquarks

2018

We propose a mechanism that allows for sizeable flavour violation in quark-lepton currents, while suppressing flavour changing neutral currents in quark-quark and lepton-lepton sectors. The mechanism is applied to the recently proposed 4321 renormalizable model, which can accommodate the current experimental anomalies in $B$-meson decays, both in charged and neutral currents, while remaining consistent with all other indirect flavour and electroweak precision measurements and direct searches at high-$p_T$. To support this claim, we present an exhaustive phenomenological survey of this fully calculable UV complete model and highlight the rich complementarity between indirect and direct searc…

Particle physicsNuclear and High Energy Physics530 PhysicsHigh Energy Physics::LatticeFlavourFOS: Physical sciences10192 Physics Institute01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHeavy Quark Physicslcsh:Nuclear and particle physics. Atomic energy. Radioactivity3106 Nuclear and High Energy Physics010306 general physicsParticle Physics - PhenomenologyPhysicshep-ex010308 nuclear & particles physicsComputer Science::Information RetrievalElectroweak interactionHigh Energy Physics::Phenomenologyhep-phComplementarity (physics)High Energy Physics - PhenomenologyGauge SymmetryBeyond Standard Modellcsh:QC770-798High Energy Physics::ExperimentParticle Physics - ExperimentBeyond Standard Model; Gauge Symmetry; Heavy Quark Physics
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Three Duality Symmetries between Photons and Cosmic String Loops, and Macro and Micro Black Holes

2015

We present a review of two thermal duality symmetries between two different kinds of systems: photons and cosmic string loops, and macro black holes and micro black holes, respectively. It also follows a third joint duality symmetry amongst them through thermal equilibrium and stability between macro black holes and photon gas, and micro black holes and string loop gas, respectively. The possible cosmological consequences of these symmetries are discussed.

Particle physicsPhysics and Astronomy (miscellaneous)General MathematicsAstrophysics::High Energy Astrophysical PhenomenaDuality (optimization)cosmic string loopDuality symmetryString (physics)black holes thermodynamicsMicro black holeGeneral Relativity and Quantum Cosmologyblack holes thermodynamicComputer Science (miscellaneous)photonsSettore MAT/07 - Fisica MatematicaBlack hole thermodynamicsduality symmetryPhysicsPhotonslcsh:MathematicsphotonPhoton gasCosmic string loopslcsh:QA1-939Black holeCosmic stringChemistry (miscellaneous)photons; cosmic string loops; black holes thermodynamics; duality symmetryBlack holes thermodynamicscosmic string loopsHawking radiation
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Lepton Number Violation in Higgs Decay at LHC

2015

We show that within the Left-Right symmetric model, lepton number violating decays of the Higgs boson can be discovered at the LHC. The process is due to the mixing of the Higgs with the triplet that breaks parity. As a result, the Higgs can act as a gateway to the origin of heavy Majorana neutrino mass. To assess the LHC reach, a detailed collider study of the same-sign di-leptons plus jets channel is provided. This process is complementary to the existing nuclear and collider searches for lepton number violation and can probe the scale of parity restoration even beyond other direct searches.

Particle physicsPhysics::Instrumentation and DetectorsPhysics beyond the Standard ModelSymmetric modelFOS: Physical sciencesGeneral Physics and AstronomyLepton number violation Higgs Large Hadron Collider left-right symmetryHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)left-right symmetryPhysicsLepton number violationLarge Hadron ColliderPhysicsHigh Energy Physics::PhenomenologyParity (physics)Lepton number3. Good healthMAJORANAHigh Energy Physics - PhenomenologyLepton number violation; Higgs; Large Hadron Collider; left-right symmetryLarge Hadron ColliderHiggs bosonHigh Energy Physics::ExperimentNeutrinoparticle physics ; higgs ; neutrinoHiggHiggsPhysical Review Letters
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Vector boson scattering: Recent experimental and theory developments

2018

This document summarises the talks and discussions happened during the VBSCan Split17 workshop, the first general meeting of the VBSCan COST Action network. This collaboration is aiming at a consistent and coordinated study of vector-boson scattering from the phenomenological and experimental point of view, for the best exploitation of the data that will be delivered by existing and future particle colliders.

Particle physicsStandard ModelGeneral Physics and AstronomyFOS: Physical sciencesvector boson: scatteringEWSB (Electroweak symmetry breaking); HEP; LHC; Standard Model; VBSLHC VBS HEP Standard Model EWSB (Electroweak symmetry breaking)01 natural sciences114 Physical sciencesVector bosonHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Point (geometry)Cost actionVBS010306 general physicsactivity reportParticle Physics - PhenomenologyPhysics010308 nuclear & particles physicsScatteringhep-exhep-phlcsh:QC1-999HEPHigh Energy Physics - PhenomenologyEWSB (Electroweak symmetry breaking)[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]networkLHClcsh:PhysicsParticle Physics - Experiment
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Effects of triplet Higgs bosons in long baseline neutrino experiments

2018

The triplet scalars $(\Delta=\Delta^{++},\Delta^{+},\Delta^{0})$, utilized in the so-called Type-II seesaw model to explain the lightness of neutrinos, would generate nonstandard interactions (NSI) for neutrino propagating in matter. We investigate the prospects to probe these interactions in long baseline neutrino oscillation experiments. We analyze the upper bounds that the proposed DUNE experiment might set on the nonstandard parameters and numerically derive upper bounds, as function of the lightest neutrino mass, on the ratio the mass $M_\Delta$ of the triplet scalars and strength $|\lambda_\phi|$ of the coupling $\phi\phi\Delta$ of the triplet $\Delta$ and conventional Higgs doublet $…

Particle physicsVIOLATIONPontecorvo–Maki–Nakagawa–Sakata matrixFOS: Physical scienceshiukkasfysiikkaComputer Science::Digital Libraries114 Physical sciences7. Clean energy01 natural sciencesHigh Energy Physics - Phenomenology (hep-ph)effective field theory0103 physical sciences010306 general physicsNeutrino oscillationBosonPhysicsLEFT-RIGHT SYMMETRYneutrino oscillationsPARITYta114010308 nuclear & particles physicsHiggsin bosoniHigh Energy Physics::PhenomenologyneutriinotParity (physics)Coupling (probability)extensions of Higgs sectorHigh Energy Physics - PhenomenologyHiggsin bosonitHiggs bosonDOUBLY-CHARGED HIGGSHigh Energy Physics::ExperimentNeutrinoLepton
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Search for supersymmetry with gauge-mediated breaking in diphoton events at D0

2004

We report the results of a search for supersymmetry (SUSY) with gauge-mediated breaking in the missing transverse energy distribution of inclusive diphoton events using 263 pb$^{-1}$ of data collected by the D0 experiment at the Fermilab Tevatron Collider in 2002--2004. No excess is observed above the background expected from standard model processes, and lower limits on the masses of the lightest neutralino and chargino of about 108 and 195 GeV, respectively, are set at the 95% confidence level. These are the most stringent limits to date for models with gauge-mediated SUSY breaking with a short-lived neutralino as the next-lightest SUSY particle.

Particle physicsstandard modelTevatronGeneral Physics and AstronomyFOS: Physical sciencessparticles01 natural sciencesStandard ModelHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics::TheoryChargino0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Grand Unified Theory14.80.Ly 12.60.Jv 13.85.RmSymmetry breaking010306 general physicsPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologySuperpartnerspontaneous symmetry breakingSupersymmetryNeutralinoHigh Energy Physics::Experimentsupersymmetry
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CP Violation in Correlated Production and Decay of Unstable Particles

2011

We study resonant CP-violating Einstein--Podolsky--Rosen correlations that may take place in the production and decay of unstable scalar particles at high-energy colliders. We show that as a consequence of unitarity and CPT invariance of the S-matrix, in 2 --> 2 scatterings mediated by mixed scalar particles, at least three linearly independent decay matrices associated with the unstable scalar states are needed to obtain non-zero CP-odd observables that are also odd under C-conjugation. Instead, for the correlated production and decay of two unstable particle systems in 2 --> 4 processes, we find that only two independent decay matrices are sufficient to induce a net non-vanishing CP…

Particle systemPhysicsNuclear and High Energy PhysicsParticle physicsUnitarityBranching fractionCPT symmetryScalar (mathematics)FOS: Physical sciencesObservableHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)CP violationHigh Energy Physics::ExperimentMinimal Supersymmetric Standard ModelParticle Physics - Phenomenology
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Does Ligand Symmetry Play a Role in the Stabilization of DNA G-Quadruplex Host-Guest Complexes?

2014

In efforts to find agents with improved biological activity against cancer cells, recent years have seen an increased interest in the study of small molecules able to bind the deoxyribonucleic acid (DNA) when it assumes secondary structures known as G-quadruplexes (G4s) preferring them over the B form. Currently, several compounds reported in literature have already shown to be good candidates as G4s DNA stabilizers. Even though some specific features for the G4s affinity are known, such as a π-delocalized system able to stack at the top/end of a G-tetrad and positively charged substituents able to interact with the grooves, it is not clear yet what kind of structural features affect more t…

PharmacologyGene isoformLigandStereochemistryOrganic ChemistryAntineoplastic AgentsDNATelomereLigandsG-quadruplexSettore CHIM/08 - Chimica FarmaceuticaBiochemistrySmall moleculeG-Quadruplexeschemistry.chemical_compoundOrder (biology)chemistrySettore CHIM/03 - Chimica Generale E InorganicaAnticancer drugs DNA G-quadruplex host-guest complexes ligand symmetry point group symmetryDrug DiscoveryMolecular symmetryHumansMolecular MedicineDNAStabilizer (chemistry)Current Medicinal Chemistry
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Intranukleäre virusähnliche Partikeln in einem Mammakarzinom

1969

By electron microscopic examination of a solid, chiefly scirrhous mammary cancer, 3 kinds of unusual nuclear inclusions were found: (a) Electron dense particles of a 54–80 nm diameter, whose outlines appear mainly hexagonal, which points at an icosahedral structure, (b) Clusters of granules with a diameter of 200–300a, respectively 300–400a, at whose circumference the larger particles appear, (c) Bundles of filaments in close association and continuous with the granules. In all 3 nuclear inclusions there are subunits of 40–45a. The comparison between these results and experiments published suggest that these nuclear inclusions are (a) virus particles, (b) virus at an early stage of developm…

PharmacologybiologyChemistryViroidIcosahedral symmetryHexagonal crystal systemCell Biologybiology.organism_classificationVirusCellular and Molecular NeuroscienceCrystallographyMolecular MedicineMolecular BiologyElectron microscopicVirus ProteinExperientia
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Genetic Normalized Convolution

2011

Normalized convolution techniques operate on very few samples of a given digital signal and add missing information, trough spatial interpolation. From a practical viewpoint, they make use of data really available and approximate the assumed values of the missing information. The quality of the final result is generally better than that obtained by traditional filling methods as, for example, bilinear or bicubic interpolations. Usually, the position of the samples is assumed to be random and due to transmission errors of the signal. Vice versa, we want to apply normalized convolution to compress data. In this case, we need to arrange a higher density of samples in proximity of zones which c…

Phase congruencyCorrectnessSettore INF/01 - InformaticaPosition (vector)Genetic algorithmGenetic Algorithms Normalized Convolution Symmetry Transform Structural Similarity Metrics Phase CongruencyBicubic interpolationBilinear interpolationDigital signal (signal processing)AlgorithmMathematicsMultivariate interpolation
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