Search results for "Arms"

showing 10 items of 182 documents

A three body state with J=3 in the ρB*B̅N* interaction

2016

We study the ρB * BN * system solving the Faddeev equations in the fixed center approximation. The B * BN * system will be considered forming a cluster, and using the two-body ρB * unitarized scattering amplitudes in the local Hidden Gauge approach we find a new I ( J PC ) = 1(3 −− ) state. The mass of the new state corresponds to a two particle invariant mass of the ρB * system close to the resonant energy of the B * 2 (5747), indicating that the role of this J = 2 resonance is important in the dynamical generation of the new state.

PhysicsFaddeev equations010308 nuclear & particles physicsPhysicsQC1-999PropagatorState (functional analysis)Gauge (firearms)01 natural sciencesResonance (particle physics)Scattering amplitudeTheoretical physics0103 physical sciencesInvariant mass010306 general physicsS-matrixMathematical physicsEPJ Web of Conferences
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An educational path for the magnetic vector potential and its physical implications

2013

We present an educational path for the magnetic vector potential A aimed at undergraduate students and pre-service physics teachers. Starting from the generalized Ampere–Laplace law, in the framework of a slowly varying time-dependent field approximation, the magnetic vector potential is written in terms of its empirical references, i.e. the conduction currents. Therefore, once the currents are known, our approach allows for a clear and univocal physical determination of A, overcoming the mathematical indeterminacy due to the gauge transformations. We have no need to fix a gauge, since for slowly varying time-dependent electric and magnetic fields, the ‘natural’ gauge for A is the Coulomb o…

PhysicsField (physics)Physics - Physics EducationClassical Physics (physics.class-ph)FOS: Physical sciencesGeneral Physics and AstronomyPhysics - Classical PhysicsGauge (firearms)Indeterminacy (literature)Magnetic fieldInterpretation (model theory)Theoretical physicsPhysics Education (physics.ed-ph)Path (graph theory)CoulombMagnetic potential
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On the relation between 2+1 Einstein gravity and Chern Simons theory

1999

A simple example is given to show that the gauge equivalence classes of physical states in Chern Simons theory are not in one-to-one correspondence with those of Einstein gravity in three spacetime dimensions. The two theories are therefore not equivalent. It is shown that including singular metrics into general relativity has more, and in fact a quite counter-intuitive, impact on the theory than one naively expects.

PhysicsGravity (chemistry)Physics and Astronomy (miscellaneous)SpacetimeGeneral relativityChern–Simons theoryFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)Gauge (firearms)General Relativity and Quantum CosmologyTheoretical physicssymbols.namesakeGeneral Relativity and Quantum CosmologyHigh Energy Physics::TheorySimple (abstract algebra)symbolsEinsteinRelation (history of concept)
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No-scale D=5 supergravity from Scherk-Schwarz reduction of D=6 theories

2004

We perform a generalized dimensional reduction of six dimensional supergravity theories to five dimensions. We consider the minimal $(2,0)$ and the maximal $(4,4)$ theories. In each case the reduction allows us to obtain gauged supergravities of no-scale type in dimension five with gauge groups that escape previous classifications. In the minimal case, the geometric data of the reduced theory correspond to particular cases of the D=5 real special geometry. In the maximal case we find a four parameter solution which allows partial breaking of supersymmetry.

PhysicsHigh Energy Physics - TheoryNuclear and High Energy PhysicsScale (ratio)SupergravityDimension (graph theory)High Energy Physics::PhenomenologyFOS: Physical sciencesFísicaSupersymmetryGauge (firearms)Type (model theory)Reduction (complexity)High Energy Physics::TheoryHigh Energy Physics - Theory (hep-th)Dimensional reductionParticle Physics - TheoryMathematical physics
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A Model of Comprehensive Unification

2017

Comprehensive – that is, gauge and family – unification using spinors has many attractive features, but it has been challenged to explain chirality. Here, by combining an orbifold construction with more traditional ideas, we address that difficulty. Our candidate model features three chiral families and leads to an acceptable result for quantitative unification of couplings. A potential target for accelerator and astronomical searches emerges.

PhysicsHigh Energy Physics - TheoryNuclear and High Energy PhysicsSpinorUnification010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesGauge (firearms)01 natural scienceslcsh:QC1-999Theoretical physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)0103 physical sciences010306 general physicsChirality (chemistry)lcsh:PhysicsOrbifold
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Measurement of theZZProduction Cross Section and Limits on Anomalous Neutral Triple Gauge Couplings in Proton-Proton Collisions ats=7  TeVwith the AT…

2012

A measurement of the ZZ production cross section in proton-proton collisions at root s = 7 TeV using data corresponding to an integrated luminosity of 1.02 fb(-1) recorded by the ATLAS experiment a ...

PhysicsLuminosity (scattering theory)Proton010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaATLAS experimentRoot (chord)General Physics and AstronomyGauge (firearms)01 natural sciencesNuclear physicsCross section (physics)medicine.anatomical_structureAtlas (anatomy)Phase space0103 physical sciencesmedicinePhysics::Accelerator PhysicsHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsPhysical Review Letters
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Set of sum rules for anomalous gauge boson couplings

1999

The dependence of the differential cross-section for on-shell W-pair production on the anomalous trilinear gauge couplings invariant under C and P is examined. It is shown that the contributions of the anomalous magnetic moments of the W boson due to the photon and the Z can be individually projected out by means of two appropriately constructed polynomials. The remaining four anomalous couplings are shown to satisfy a set of model-independent sum rules. Specific models which predict special relations among the anomalous couplings are then studied; in particular, the composite model of Brodsky and Hiller, and the linear and non-linear effective Lagrangian approaches. The relations predicted…

PhysicsNuclear and High Energy PhysicsGauge bosonParticle physicsPhotonElectron–positron annihilationForm factor (quantum field theory)FOS: Physical sciencesFísicaGauge (firearms)Theoretical physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)BibliographySum rule in quantum mechanicsInvariant (mathematics)Particle Physics - Phenomenology
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Hefty MSSM-like light Higgs in extended gauge models

2011

It is well known that in the MSSM the lightest neutral Higgs h^0 must be, at the tree level, lighter than the Z boson and that the loop corrections shift this stringent upper bound up to about 130 GeV. Extending the MSSM gauge group in a suitable way, the new Higgs sector dynamics can push the tree-level mass of h^0 well above the tree-level MSSM limit if it couples to the new gauge sector. This effect is further pronounced at the loop level and h^0 masses in the 140 GeV ballpark can be reached easily. We exemplify this for a sample setting with a low-scale U(1)_R x U(1)_B-L gauge symmetry in which neutrino masses can be implemented via the inverse seesaw mechanism.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaGauge (firearms)01 natural sciencesUpper and lower boundsHiggs sectorHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologySeesaw mechanismHigh Energy Physics - Phenomenology (hep-ph)Gauge group0103 physical sciencesHiggs bosonHigh Energy Physics::ExperimentNeutrino010306 general physicsGauge symmetry
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B-L-violating masses in softly broken supersymmetry

1997

We prove a general low-energy theorem establishing a generic relation between the neutrino Majorana mass and the superpartner sneutrino B-L-violating "Majorana"-like mass term. The theorem states that, if one of these two quantities is non-zero the other one is also non-zero and, vice versa, if one of them vanishes the other vanishes, too. The theorem is a consequence of the underlying supersymmetry (SUSY) and valid for any realistic gauge model with weak scale softly broken SUSY.

PhysicsNuclear and High Energy PhysicsParticle physicsB − LHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesSuperpartnerScale (descriptive set theory)SupersymmetryGauge (firearms)High Energy Physics - PhenomenologyHigh Energy Physics::TheoryMAJORANAHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentNeutrinoPhysics Letters B
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CP-violation with bosons

1993

We formulate the conditions under which a purely bosonic theory (without fermions) containing neutral spin-0 particles and vector (gauge) bosons violates the CP-symmetry through the presence of CP-even and CP-odd operators in the Lagrangian. This is done without reference to explicitly CP-violating scalar sector of extended standard models (SM) with two or more Higgs doublets. The Lagrangian expressed in the mass basis of the spin-0 fields can, however, in certain cirumstances be identified with a part of the CP-violating SM with two Higgs doublets. It is instructive to consider the manifestation of CP-violation in the mass basis since this leads directly to suggestions of genuine CP-signal…

PhysicsNuclear and High Energy PhysicsParticle physicsBasis (linear algebra)High Energy Physics::PhenomenologyScalar (mathematics)FOS: Physical sciencesFermionGauge (firearms)High Energy Physics - Phenomenologysymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)symbolsHiggs bosonCP violationLagrangianBosonPhysics Letters B
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