Search results for "Spinor"

showing 10 items of 36 documents

Higher Order Integrability in Generalized Holonomy

2004

Supersymmetric backgrounds in M-theory often involve four-form flux in addition to pure geometry. In such cases, the classification of supersymmetric vacua involves the notion of generalized holonomy taking values in SL(32,R), the Clifford group for eleven-dimensional spinors. Although previous investigations of generalized holonomy have focused on the curvature \Rm_{MN}(\Omega) of the generalized SL(32,R) connection \Omega_M, we demonstrate that this local information is incomplete, and that satisfying the higher order integrability conditions is an essential feature of generalized holonomy. We also show that, while this result differs from the case of ordinary Riemannian holonomy, it is n…

PhysicsHigh Energy Physics - TheoryNuclear and High Energy PhysicsPure mathematicsSpinorWilson loopHolonomyLie groupFOS: Physical sciencesSupersymmetrySymmetry groupCurvatureConnection (mathematics)High Energy Physics - Theory (hep-th)Mathematics::Differential Geometry
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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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Lagrangians for Massive Dirac Chiral Superfields

2016

A variant for the superspin one-half massive superparticle in $ 4D $, $ \mathcal{N}=1 $, based on Dirac superfields, is offered. As opposed to the current known models that use spinor chiral superfields, the propagating fields of the supermultiplet are those of the lowest mass dimensions possible: scalar, Dirac and vector fields. Besides the supersymmetric chiral condition, the Dirac superfields are not further constrained, allowing a very straightforward implementation of the path-integral method. The corresponding superpropagators are presented. In addition, an interaction super Yukawa potential, formed by Dirac and scalar chiral superfields, is given in terms of their component fields. T…

PhysicsHigh Energy Physics - TheoryParticle physicsNuclear and High Energy PhysicsCurrent (mathematics)Spinor010308 nuclear & particles physicsOperator (physics)High Energy Physics::LatticeDirac (software)Scalar (mathematics)High Energy Physics::PhenomenologyYukawa potentialFOS: Physical sciences01 natural sciencesMAJORANAHigh Energy Physics::TheoryHigh Energy Physics - Theory (hep-th)Supermultiplet0103 physical sciences010306 general physicsMathematical physics
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Enumerating higher-dimensional operators with on-shell amplitudes

2020

We establish a simple formula for the minimal dimension of operators leading to any helicity amplitude. It eases the systematic enumeration of independent operators from the construction of massless non-factorizable on-shell amplitudes. Little-group constraints can then be solved algorithmically for each helicity configuration to extract a complete set of spinor structures with lowest dimension. Occasionally, further reduction using momentum conservation, on-shell conditions and Schouten identities is required. A systematic procedure to account for the latter is presented. Dressing spinor structures with dot products of momenta finally yields the independent Lorentz structures for each heli…

PhysicsHigh Energy Physics - TheorySpinor010308 nuclear & particles physicsLorentz transformationGravitonFOS: Physical sciencesComputer Science::Digital Libraries01 natural sciencesHelicitysymbols.namesakeHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)Dimension (vector space)0103 physical sciencessymbolsEffective field theory010306 general physicsMathematical physicsGauge symmetrySpin-½
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Dynamics for a simple graph using the U(N) framework for loop quantum gravity

2012

The implementation of the dynamics in loop quantum gravity (LQG) is still an open problem. Here, we discuss a tentative dynamics for the simplest class of graphs in LQG: Two vertices linked with an arbitrary number of edges. We find an interesting global U(N) symmetry in this model that selects the homogeneous/isotropic sector. Then, we propose a quantum Hamiltonian operator for this reduced sector. Finally, we introduce the spinor representation for LQG in order to propose a classical effective dynamics for this model.

PhysicsHistorySpinorOpen problemFOS: Physical sciencesLoop quantum gravityGeneral Relativity and Quantum Cosmology (gr-qc)Linear-quadratic-Gaussian controlGeneral Relativity and Quantum CosmologySymmetry (physics)Computer Science ApplicationsEducationTheoretical physicsComputer Science::Systems and ControlQuantum gravityddc:530Representation (mathematics)Quantum
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Lorentz Multiplet Structure of Baryon Spectra and Relativistic Description

1997

The pole positions of the various baryon resonances are known to reveal well-pronounced clustering, so-called Hoehler clusters. For nonstrange baryons the Hoehler clusters are shown to be identical to Lorentz multiplets of the type (j,j)*[(1/2,0)+(0,1/2)] with j being a half-integer. For the Lambda hyperons below 1800 MeV these clusters are shown to be of the type [(1,0)+ (0,1)]*[(1/2,0)+(0,1/2)] while above 1800 MeV they are parity duplicated (J,0)+(0,J) (Weinberg-Ahluwalia) states. Therefore, for Lambda hyperons the restoration of chiral symmetry takes place above 1800 MeV. Finally, it is demonstrated that the description of spin-3/2 particles in terms of a 2nd rank antisymmetric Lorentz …

PhysicsNuclear and High Energy PhysicsNuclear TheoryAntisymmetric relationLorentz transformationNuclear TheoryHyperonFOS: Physical sciencesGeneral Physics and AstronomyAstronomy and AstrophysicsParity (physics)Spectral lineNuclear Theory (nucl-th)BaryonHigh Energy Physics - Phenomenologysymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)Dirac spinorsymbolsMultipletMathematical physicsModern Physics Letters A
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Supersymmetry in the standard model of electroweak interactions

1993

Abstract Starting from the peculiar chirality pattern of weak and electromagnetic interactions, established by experiment, we show that the minimal standard model contains supersymmetry, though in a new, unconventional, realization. It appears as an action on the fields but is not an invariance of the lagrangian. This supersymmetry which is not in conflict with experiment, is seen to be the raison d'etre of the Higgs fields and provides a geometrical understanding of spontaneous symmetry breaking. It turns out that this approach which is based on the fundamental role of left- and right-chiral spinor fields in weak interactions, has many similarities to models developed in the framework of n…

PhysicsNuclear and High Energy PhysicsParticle physicsTheoretical physicsSpinorSpontaneous symmetry breakingHigh Energy Physics::PhenomenologyElectroweak interactionHiggs bosonSupersymmetrySupersymmetry breakingNoncommutative geometryStandard ModelPhysics Letters B
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Light-by-light scattering sum rules constraining meson transition form factors

2012

Relating the forward light-by-light scattering to energy weighted integrals of the \gamma* \gamma -fusion cross sections, with one real photon (\gamma) and one virtual photon (\gamma*), we find two new exact super-convergence relations. They complement the known super-convergence relation based on the extension of the GDH sum rule to the light-light system. We also find a set of sum rules for the low-energy photon-photon interaction. All of the new relations are verified here exactly at leading order in scalar and spinor QED. The super-convergence relations, applied to the \gamma* \gamma -production of mesons, lead to intricate relations between the \gamma \gamma -decay widths or the \gamma…

PhysicsNuclear and High Energy PhysicsSpinorMesonNuclear TheoryAstrophysics::High Energy Astrophysical PhenomenaNuclear TheoryScalar (mathematics)High Energy Physics::PhenomenologyOrder (ring theory)Virtual particleFOS: Physical sciencesNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Quantum mechanicsProduction (computer science)High Energy Physics::ExperimentSum rule in quantum mechanicsEnergy (signal processing)Mathematical physics
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Use of helicity methods in evaluating loop integrals: A QCD example

1991

We discuss the use of helicity methods in evaluating loop diagrams by analyzing a specific example: the one-loop contribution to e+e- → qqg in massless QCD. By using covariant helicity representations for the spinor and vector wave functions we obtain the helicity amplitudes directly from the Feynman loop diagrams by covariant contraction. The necessary loop integrations are considerably simplified since one encounters only scalar loop integrals after contraction. We discuss crossing relations that allow one to obtain the corresponding one-loop helicity amplitudes for the crossed processes as e.g. qq → (W, Z, γ∗) + g including the real photon cases. As we treat the spin degrees of freedom i…

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsSpinorScalar (mathematics)Helicitysymbols.namesakeDimensional regularizationDimensional reductionQuantum electrodynamicssymbolsFeynman diagramCovariant transformationMathematical physicsNuclear Physics B
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Matter-wave interference versus spontaneous pattern formation in spinor Bose-Einstein condensates

2013

We describe effects of matter-wave interference of spinor states in the $^{87}$Rb Bose-Einstein condensate. The components of the F=2 manifold are populated by forced Majorana transitions and then fall freely due to gravity in an applied magnetic field. Weak inhomogeneities of the magnetic field, present in the experiment, impose relative velocities onto different $m_F$ components, which show up as interference patterns upon measurement of atomic density distributions with a Stern-Gerlach imaging method. We show that interference effects may appear in experiments even if gradients of the magnetic field components are eliminated but higher order inhomogeneity is present and the duration of t…

PhysicsSpinorFOS: Physical sciencesPattern formationInterference (wave propagation)Atomic and Molecular Physics and OpticsManifoldMagnetic fieldlaw.inventionMAJORANAQuantum Gases (cond-mat.quant-gas)lawQuantum mechanicsMatter waveCondensed Matter - Quantum GasesBose–Einstein condensatePhysical Review A
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