Search results for "Monopole"

showing 10 items of 76 documents

Magnetic Monopole Search with the Full MoEDAL Trapping Detector in 13 TeV pp Collisions Interpreted in Photon-Fusion and Drell-Yan Production

2019

MoEDAL is designed to identify new physics in the form of stable or pseudostable highly ionizing particles produced in high-energy Large Hadron Collider (LHC) collisions. Here we update our previous search for magnetic monopoles in Run 2 using the full trapping detector with almost four times more material and almost twice more integrated luminosity. For the first time at the LHC, the data were interpreted in terms of photon-fusion monopole direct production in addition to the Drell-Yan-like mechanism. The MoEDAL trapping detector, consisting of 794 kg of aluminum samples installed in the forward and lateral regions, was exposed to 4.0 fb$^{-1}$ of 13 TeV proton-proton collisions at the LHC…

General PhysicsPhotonPhysics beyond the Standard ModelPhysics MultidisciplinaryMagnetic monopoleGeneral Physics and AstronomyFOS: Physical sciencesddc:500.27. Clean energy01 natural sciences114 Physical sciencesMoEDAL Collaboration09 EngineeringHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)STOPPING-POWER0103 physical sciences010306 general physicsPROTON COLLISIONS01 Mathematical SciencesParticle Physics - PhenomenologyPhysicsLarge Hadron ColliderLuminosity (scattering theory)Science & Technology02 Physical SciencesMagnetic monopoleInteraction pointhep-exDirac (video compression format)PhysicsCharge (physics)hep-phHigh Energy Physics - PhenomenologyPhysical SciencesLHCParticle Physics - Experiment
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Geometric quantization in the presence of an electromagnetic field

1983

Some aspects of the formalism of geometric quantization are described emphasizing the role played by the symmetry group of the quantum system which, for the free particle, turns out to be a central extensionG(m) of the Galilei groupG. The resulting formalism is then applied to the case of a particle interacting with the electromagnetic field, which appears as a necessary modification of the connection 1-form of the quantum bundle when its invariance group is generalized to alocal extension ofG. Finally, the quantization of the electric charge in the presence of a Dirac monopole is also briefly considered.

Geometric quantizationPhysicsQuantization (physics)Free particleClassical mechanicsPhysics and Astronomy (miscellaneous)Canonical quantizationGeneral MathematicsMagnetic monopoleQuantum field theoryQuantumSecond quantizationInternational Journal of Theoretical Physics
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Gravitational scattering on a global monopole

1991

The scattering amplitude and the total scattering cross section of massless particles propagating in the gravitational field of a global monopole are derived. We find that the physical signature of such defects is a ringlike angular region where the scattering amplitude is very large. The size of this ringlike region is determined by the ratio of the global monopole mass to the Planck mass and its appearance stems from the fact that the metric of the global monopole is not asymptotically flat but rather displays the characteristic spherical angle defect. The situation is therefore very much reminiscent of scattering in the gravitational field of the cosmic string.

GravitationCosmic stringScattering amplitudeMassless particlePhysicsGravitational fieldScatteringQuantum mechanicsPlanck massMagnetic monopoleFísica
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Searching for long-lived particles beyond the Standard Model at the Large Hadron Collider

2020

Particles beyond the Standard Model (SM) can generically have lifetimes that are long compared to SM particles at the weak scale. When produced at experiments such as the Large Hadron Collider (LHC) at CERN, these longlived particles (LLPs) can decay far from the interaction vertex of the primary proton–proton collision. Such LLP signatures are distinct from those of promptly decaying particles that are targeted by the majority of searches for new physics at the LHC, often requiring customized techniques to identify, for example, significantly displaced decay vertices, tracks with atypical properties, and short track segments. Given their non-standard nature, a comprehensive overview of LLP…

HIGH-ENERGYbeyond the Standard Modellarge hadron colliderPhysics::Instrumentation and DetectorsPROTON-PROTON COLLISIONSPhysics beyond the Standard Modelbeyond the standard model01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)high-luminosity lhcHigh Energy Physics - Phenomenology (hep-ph)MAGNETIC MONOPOLESlong-lived [particle]high-energy collider experimentsdecay: vertexscattering [p p][PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]long-lived particlesQCproposed [detector]Physicslifetimedark gauge forcesLarge Hadron ColliderCMSROOT-S=13 TEVroot-s=13 tevPhysicsnew physics: search forscale: electroweak interactionhep-phATLASelectroweak interaction [scale]vertex [decay]upgrade [detector]High Energy Physics - Experiment; High Energy Physics - Experiment; High Energy Physics - Phenomenologydetector: upgradeSettore FIS/02 - Fisica Teorica Modelli e Metodi Matematiciprimary [vertex]ddc:High Energy Physics - PhenomenologyCERN LHC CollLarge Hadron Colliderbaryon asymmetryvertex: primaryLHCcolliding beams [p p]exclusion limitspp collisionsParticle Physics - ExperimentsignatureNuclear and High Energy PhysicsParticle physicsp p: scatteringCERN LabPAIR PRODUCTIONcollider phenomenologyreviewFOS: Physical sciencesDARK GAUGE FORCES530search for [new physics]BARYON ASYMMETRY0103 physical sciencesddc:530010306 general physicsnumerical calculationsParticle Physics - PhenomenologyEXCLUSION LIMITSmagnetic monopolesPP COLLISIONS010308 nuclear & particles physicshep-exbackgroundbibliographyshowersMAJORANA NEUTRINOSCollisiontracksLHC-Bdetector: proposedhigh-luminosity LHCpair productionMATHUSLAPhysics and Astronomy[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]proton-proton collisionshigh-energymajorana neutrinosparticle: long-livedp p: colliding beamsPhysics BSMexperimental results
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Small and hollow magnetic monopoles

2018

We deal with the presence of magnetic monopoles in a non Abelian model that generalizes the standard 't~Hooft-Polyakov model in three spatial dimensions. We investigate the energy density of the static and spherically symmetric solutions to find first order differential equations that solve the equations of motion. The system is further studied and two distinct classes of solutions are obtained, one that can also be described by analytical solutions which is called small monopole, since it is significantly smaller than the standard 't~Hooft-Polyakov monopole. The other type of structure is the hollow monopole, since the energy density is endowed with a hole at its core. The hollow monopole …

High Energy Physics - TheoryPhysics010308 nuclear & particles physicsDifferential equationHigh Energy Physics::LatticeMathematical analysisMagnetic monopoleStructure (category theory)FOS: Physical sciencesEquations of motionPattern Formation and Solitons (nlin.PS)Type (model theory)Nonlinear Sciences - Pattern Formation and Solitons01 natural sciencesCondensed Matter - Other Condensed MatterCore (optical fiber)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)Ordinary differential equation0103 physical sciencesEnergy density010306 general physicsOther Condensed Matter (cond-mat.other)Physical Review D
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Q7-branes and their coupling to IIB supergravity

2007

We show how, by making use of a new basis of the IIB supergravity axion-dilaton coset, SL(2,R)/SO(2), 7-branes that belong to different conjugacy classes of the duality group SL(2,R) naturally couple to IIB supergravity with appropriate source terms characterized by an SL(2,R) charge matrix Q. The conjugacy classes are determined by the value of the determinant of Q. The (p,q) 7-branes are the branes in the conjugacy class detQ = 0. The 7-branes in the conjugacy class detQ > 0 are labelled by three numbers (p,q,r) which parameterize the matrix Q and will be called Q7-branes. We construct the full bosonic Wess--Zumino term for the Q7-branes. In order to realize a gauge invariant coupling …

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsPure mathematicsSupergravityFOS: Physical sciencesMONOPOLESInvariant (physics)p-branesBRANESFIELDSINSTANTONSABELIAN BORN-INFELDConjugacy classDOMAIN-WALLSHigh Energy Physics - Theory (hep-th)DUALITYD-branesBrane cosmologyCoset6 DIMENSIONS
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Dynamical Abelian Projection of Gluodynamics

1996

Assuming the monopole dominance, that has been proved in the lattice gluodynamics, to hold in the continuum limit, we develop an effective scalar field theory for QCD at large distances to describe confinement. The approach is based on a gauge (or projection) independent formulation of the monopole dominance and manifestly Lorentz invariant.

High Energy Physics - TheoryQuantum chromodynamicsPhysicsNuclear and High Energy PhysicsScalar field theoryContinuum (measurement)High Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)Magnetic monopoleFOS: Physical sciencesLorentz covarianceAtomic and Molecular Physics and OpticsHigh Energy Physics - LatticeHigh Energy Physics - Theory (hep-th)Lattice (order)Abelian groupMathematical physics
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"Table 1" of "Search for magnetic monopoles in sqrt(s) = 7 TeV pp collisions with the ATLAS detector"

2013

Efficiency versus transverse kinetic energy, averaged over |eta|<1.37, for single monopoles of mass 200 GeV and 1500 GeV.

InclusiveEFFICIENCYProton-Proton ScatteringAstrophysics::High Energy Astrophysical PhenomenaP P --> MONOPOLE X7000.0High Energy Physics::ExperimentNuclear Experiment
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"Table 2" of "Search for magnetic monopoles in sqrt(s) = 7 TeV pp collisions with the ATLAS detector"

2013

Upper limits on the monopole production cross sections at 95% confidence level assuming the kinematic distributions from Drell-Yan and in the fiducial region.

InclusiveProton-Proton ScatteringNuclear TheoryHigh Energy Physics::PhenomenologyIntegrated Cross SectionP P --> MONOPOLE X7000.0High Energy Physics::ExperimentCross SectionNuclear ExperimentSIG
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Organometallic Magnetic Materials

2007

This chapter focuses on organometallic magnetic materials. It discusses the magnetic charge transfer salts based on metallocenes and hybrid magnets containing metallocenes. Polynuclear magnetic molecules based on metallocenes are also covered.

Magnetic moleculesChemical physicsChemistryMagnetInorganic chemistryMagnetic monopoleMolecule-based magnets
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