0000000000236780

AUTHOR

R. Saar

showing 4 related works from this author

"Dynamical" interactions and gauge invariance

2009

Appreciating the classical understanding of the elementary particle the "dynamical" Poincare algebra is developed. It is shown that the "dynamical" Poincare algebra and the equations of motion of particles with arbitrary spin are gauge invariant and that gauge invariance and relativistic invariance stand on equal footings. A "dynamical" non-minimal interaction is constructed explicitly and the Rarita-Schwinger equation is considered in the framework of this "dynamical" interaction.

Electromagnetic fieldPhysicsHigh Energy Physics - TheoryNuclear and High Energy PhysicsLorentz transformationHigh Energy Physics::LatticeAdjoint representationPlane waveFOS: Physical sciencesAnalysis of flowssymbols.namesakeHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Classical mechanicsHigh Energy Physics - Theory (hep-th)Dirac equationRarita–Schwinger equationsymbolsGauge theory
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Group theory aspects of chaotic strings

2014

Chaotic strings are a special type of non-hyperbolic coupled map lattices, exhibiting a rich structure of complex dynamical phenomena with a surprising correspondence to physical contents. Chaotic strings are generated by the Chebyshev maps T2() and T3(). In this paper we connect the Chebyshev maps via the Galois theory to the cyclic groups Z2 and Z3 and give some ideas how this fundamental connection might lead to the emergence of the familiar Lie group structure of particle physics and, finally, even to the emergence of space-time. The Z3-graded cubic and ternary algebras presented here have been introduced by R. Kerner in 1991 and then developed and elaborated in collaboration with many …

HistoryPure mathematicsGalois theoryChaoticStructure (category theory)Lie groupCyclic groupType (model theory)String (physics)Computer Science ApplicationsEducationAlgebraGroup theoryMathematicsJournal of Physics: Conference Series
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Mass, zero mass and ... nophysics

2017

In this paper we demonstrate that massless particles cannot be considered as limiting case of massive particles. Instead, the usual symmetry structure based on semisimple groups like $U(1)$, $SU(2)$ and $SU(3)$ has to be replaced by less usual solvable groups like the minimal nonabelian group ${\rm sol}_2$. Starting from the proper orthochronous Lorentz group ${\rm Lor}_{1,3}$ we extend Wigner's little group by an additional generator, obtaining the maximal solvable or Borel subgroup ${\rm Bor}_{1,3}$ which is equivalent to the Kronecker sum of two copies of ${\rm sol}_2$, telling something about the helicity of particle and antiparticle states.

High Energy Physics - TheoryAntiparticle010308 nuclear & particles physicsGroup (mathematics)Generator (category theory)Applied MathematicsMathematics::Classical Analysis and ODEsFOS: Physical sciencesMathematical Physics (math-ph)01 natural sciencesHelicityLorentz groupGeneral Physics (physics.gen-ph)Physics - General PhysicsHigh Energy Physics - Theory (hep-th)Borel subgroupSolvable group0103 physical sciencesSymmetry (geometry)010306 general physicsMathematical PhysicsMathematical physicsMathematics
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Lorentz invariance and gauge equivariance

2014

Trying to place Lorentz and gauge transformations on the same foundation, it turns out that the first one generates invariance, the second one equivariance, at least for the abelian case. This similarity is not a hypothesis but is supported by and a consequence of the path integral formalism in quantum field theory.

HistoryGauge bosonIntroduction to gauge theoryCPT symmetryLorentz transformationLorentz covarianceComputer Science ApplicationsEducationsymbols.namesakeClassical mechanicsLorenz gauge conditionsymbolsQuantum field theoryMathematical physicsGauge fixingMathematicsJournal of Physics: Conference Series
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