Search results for "symmetry"

showing 10 items of 3576 documents

Search for New Phenomena intt¯Events with Large Missing Transverse Momentum in Proton-Proton Collisions ats=7  TeVwith the ATLAS Detector

2012

A search for new phenomena in tt events with large missing transverse momentum in proton-proton collisions at a center-of-mass energy of 7 TeV is presented. The measurement is based on 1.04  fb-1 of data collected with the ATLAS detector at the LHC. Contributions to this final state may arise from a number of standard model extensions. The results are interpreted in terms of a model where new top-quark partners are pair produced and each decay to an on-shell top (or antitop) quark and a long-lived undetected neutral particle. The data are found to be consistent with standard model expectations. A limit at 95% confidence level is set excluding a cross section times branching ratio of 1.1 pb …

QuarkPhysicsParticle physicsLarge Hadron Collider010308 nuclear & particles physicsAtlas detectorBranching fractionGeneral Physics and AstronomySupersymmetry01 natural sciencesNuclear physics0103 physical sciencesTransverse momentumFourth generationHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsNeutral particlePhysical Review Letters
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LHC diphoton resonance from gauge symmetry

2015

Motivated by what is possibly the first sign of new physics seen at the LHC, the diphoton excess at $750$ GeV in ATLAS and CMS, we present a model that provides naturally the necessary ingredients to explain the resonance. The simplest phenomenological explanation for the diphoton excess requires a new scalar state, $X(750)$, as well as additional vector-like (VL) fermions introduced in an ad-hoc way in order to enhance its decays into a pair of photons and/or increase its production cross-section. We show that the requiered VL quarks and their couplings can emerge naturally from a complete framework based on the $SU(3)_L \otimes U(1)_\mathcal{X}$ gauge symmetry.

QuarkPhysicsParticle physicsLarge Hadron ColliderPhoton010308 nuclear & particles physicsPhysics beyond the Standard ModelScalar (mathematics)FOS: Physical sciencesFermionParameter space01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsGauge symmetryPhysical Review D
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Charge asymmetry in hadroproduction of heavy quarks

1998

A sizeable difference in the differential production cross section of top and antitop quarks, respectively, is predicted for hadronically produced heavy quarks. It is of order $\alpha_s$ and arises from the interference between charge odd and even amplitudes respectively. For the TEVATRON it amounts to approximately 5-10% in the region where the cross section is large and could therefore be measured in the next round of experiments. At the LHC the asymmetry can be studied by selecting appropriately chosen kinematical regions.

QuarkPhysicsParticle physicsLarge Hadron Collidermedia_common.quotation_subjectHigh Energy Physics::PhenomenologyTevatronFísicaGeneral Physics and AstronomyOrder (ring theory)FOS: Physical sciencesCharge (physics)AsymmetryNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Production (computer science)High Energy Physics::ExperimentFermilabmedia_common
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Molecular $\Omega_c$ states generated from coupled meson-baryon channels

2018

We have investigated $\Omega_c$ states that are dynamically generated from the meson-baryon interaction. We use an extension of the local hidden gauge to obtain the interaction from the exchange of vector mesons. We show that the dominant terms come from the exchange of light vectors, where the heavy quarks are spectators. This has as a consequence that heavy quark symmetry is preserved for the dominant terms in the $(1/m_Q)$ counting, and also that the interaction in this case can be obtained from the $\textrm{SU(3)}$ chiral Lagrangians. We show that for a standard value for the cutoff regulating the loop, we obtain two states with $J^{P}={1/2}^{-}$ and two more with $J^{P}={3/2}^{-}$, thr…

QuarkPhysicsParticle physicsMeson010308 nuclear & particles physicsHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyGauge (firearms)01 natural sciencesOmegaComputer Science::Digital LibrariesSymmetry (physics)Loop (topology)BaryonHigh Energy Physics - Phenomenology0103 physical sciences010306 general physicsNuclear Experiment
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Is the spectrum of highly excited mesons purely coulombian?

2008

We show that a static central potential may provide a precise description of highly excited light unflavoured mesons. Due to string breaking this potential becomes of chromoelectric type at sufficiently large quark-antiquark distances giving rise to a coulombian spectrum. The same conclusion can be inferred for any other meson sector through a straightforward extension of our analysis.

QuarkPhysicsParticle physicsMesonHigh Energy Physics::LatticeSpectrum (functional analysis)Nuclear TheoryHigh Energy Physics::PhenomenologyGeneral Physics and AstronomyFOS: Physical sciencesFísicaType (model theory)String theoryString (physics)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Excited stateQuantum electrodynamicsHigh Energy Physics::ExperimentSymmetry breaking
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Exotic dynamically generated baryons with C=-1

2010

We follow a model based on the SU(8) symmetry for the interaction of mesons with baryons. The model treats on an equal footing the pseudo-scalars and the vector mesons, as required by heavy quark symmetry. The T-matrix calculated within an unitary scheme in coupled channels has poles which are interpreted as baryonic resonances.

QuarkPhysicsParticle physicsMesonNuclear Theory010308 nuclear & particles physicsHigh Energy Physics::LatticeHadronNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesElementary particleSymmetry group01 natural sciencesSymmetry (physics)BaryonNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsNuclear ExperimentS-matrix
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Soft SUSY breaking grand unification: Leptons vs quarks on the flavor playground

2007

We systematically analyze the correlations between the various leptonic and hadronic flavor violating processes arising in SUSY Grand Unified Theories. Using the GUT-symmetric relations between the soft SUSY breaking parameters, we assess the impact of hadronic and leptonic flavor observables on the SUSY sources of flavor violation.

QuarkPhysicsParticle physicsNuclear and High Energy PhysicsAnomalous magnetic dipole momentCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesSupersymmetryHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Grand Unified TheoryCentre for High Energy PhysicsSoft SUSY breakingHigh Energy Physics::ExperimentMinimal Supersymmetric Standard ModelLepton
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Physical constraints on a class of two-Higgs doublet models with FCNC at tree level

2014

We analyse the constraints and some of the phenomenological implications of a class of two Higgs doublet models where there are flavour-changing neutral currents (FCNC) at tree level but the potentially dangerous FCNC couplings are suppressed by small entries of the CKM matrix V. This class of models have the remarkable feature that, as a result of a discrete symmetry of the Lagrangian, the FCNC couplings are entirely fixed in the quark sector by V and the ratio v 2/v 1 of the vevs of the neutral Higgs. The discrete symmetry is extended to the leptonic sector, so that there are FCNC in the leptonic sector with their flavour structure fixed by the leptonic mixing matrix. We analyse a large n…

QuarkPhysicsParticle physicsNuclear and High Energy PhysicsHiggs PhysicsCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::PhenomenologyStructure (category theory)FísicaFOS: Physical sciencesHigh Energy Physics - ExperimentMatrix (mathematics)High Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Higgs Physics; Beyond Standard ModelBeyond Standard ModelHiggs bosonHigh Energy Physics::ExperimentTree (set theory)Mixing (physics)Discrete symmetryJournal of High Energy Physics
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Measurement of the Forward-Backward Asymmetry in the Production ofB±Mesons inpp¯Collisions ats=1.96  TeV

2015

We present a measurement of the forward-backward asymmetry in the production of B-+/- mesons, A(FB)(B-+/-) using B-+/- -> J/ Psi K-+/- decays in 10.4 fb(-1) of p (p) over bar collisions at root s = 1.96 TeV collected by the D0 experiment during Run II of the Tevatron collider. A nonzero asymmetry would indicate a preference for a particular flavor, i.e., b quark or (b) over bar antiquark, to be produced in the direction of the proton beam. We extract A(FB) (B-+/-) from a maximum likelihood fit to the difference between the numbers of forward-and backward-produced B-+/- mesons. We measure an asymmetry consistent with zero: A(FB) (B-+/-) = [-0.24 +/- 0.41 (stat) +/- 0.19 (syst)] %.

QuarkPhysicsParticle physicsProtonMeson010308 nuclear & particles physicsmedia_common.quotation_subjectHigh Energy Physics::PhenomenologyTevatronGeneral Physics and Astronomy01 natural sciencesBottom quarkAsymmetryNuclear physics0103 physical sciencesHigh Energy Physics::ExperimentB mesonRapidity010306 general physicsmedia_commonPhysical Review Letters
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Natural quasi-alignment with two Higgs doublets and RGE stability

2015

In the context of two Higgs doublet models, we study the conditions required in order to have stable quasi-alignment in flavour space. We show that stability under the RGE imposes strong constraints on the flavour structure of the Yukawa couplings associated to each one of the Higgs doublets. In particular, we find a novel solution, where all Yukawa couplings are proportional to the so-called democratic matrix. This solution is rather unique, since it is the only stable solution which is a good starting point for reproducing the observed pattern of quark masses and mixing. We also show that this stable solution can be obtained by imposing on the Lagrangian a $Z_3 \times Z^\prime_3$ flavour …

QuarkPhysicsParticle physicsTop quarkPhysics and Astronomy (miscellaneous)High Energy Physics::LatticeHigh Energy Physics::PhenomenologyYukawa potentialFOS: Physical sciencesFísicaTop quark condensateBottom quarkHigh Energy Physics - PhenomenologyHiggs fieldHigh Energy Physics - Phenomenology (hep-ph)Higgs bosonHigh Energy Physics::ExperimentEngineering (miscellaneous)Discrete symmetryParticle Physics - PhenomenologyEuropean Physical Journal C
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