0000000000076943

AUTHOR

Mario Paschke

showing 5 related works from this author

Leptonic Generation Mixing, Noncommutative Geometry and Solar Neutrino Fluxes

1997

Triangular mass matrices for neutrinos and their charged partners contain full information on neutrino mixing in a most concise form. Although the scheme is general and model independent, triangular matrices are typical for reducible but indecomposable representations of graded Lie algebras which, in turn, are characteristic for the standard model in noncommutative geometry. The mixing matrix responsible for neutrino oscillations is worked out analytically for two and three lepton families. The example of two families fixes the mixing angle to just about what is required by the Mikheyev-Smirnov-Wolfenstein resonance oscillation of solar neutrinos. In the case of three families we classify a…

PhysicsNuclear and High Energy PhysicsParticle physicsSolar neutrinoHigh Energy Physics::PhenomenologyFOS: Physical sciencesNoncommutative geometryStandard Model (mathematical formulation)Matrix (mathematics)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentNeutrinoNeutrino oscillationMixing (physics)Lepton
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Mass relations in noncommutative geometry revisited

1997

We generalize the notion of the 'noncommutative coupling constant' given by Kastler and Sch"ucker by dropping the constraint that it commute with the Dirac-operator. This leads essentially to the vanishing of the lower bound for the Higgsmass and of the upper bound for the W-mass.

PhysicsCoupling constantConstraint (information theory)High Energy Physics - TheoryNuclear and High Energy PhysicsHigh Energy Physics - Theory (hep-th)Mathematics::Operator AlgebrasFOS: Physical sciencesUpper and lower boundsNoncommutative geometryMathematical physics
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Can (noncommutative) geometry accommodate leptoquarks?

1997

We investigate the geometric interpretation of the Standard Model based on noncommutative geometry. Neglecting the $S_0$-reality symmetry one may introduce leptoquarks into the model. We give a detailed discussion of the consequences (both for the Connes-Lott and the spectral action) and compare the results with physical bounds. Our result is that in either case one contradicts the experimental results.

Reality structurePhysicsHigh Energy Physics - TheoryNuclear and High Energy PhysicsHigh Energy Physics::PhenomenologyScalar (mathematics)FOS: Physical sciencesNoncommutative geometryAction (physics)Quantum differential calculusStandard Model (mathematical formulation)Theoretical physicsHigh Energy Physics - Theory (hep-th)Mathematics::K-Theory and HomologyHigh Energy Physics::ExperimentNoncommutative algebraic geometryNoncommutative quantum field theory
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Multiple Noncommutative Tori and Hopf Algebras

2001

We derive the Kac-Paljutkin finite-dimensional Hopf algebras as finite fibrations of the quantum double torus and generalize the construction for quantum multiple tori.

PhysicsPure mathematicsAlgebra and Number TheoryFOS: Physical sciencesTorusMathematics - Rings and AlgebrasMathematical Physics (math-ph)Hopf algebraNoncommutative geometry16W30 57T05Rings and Algebras (math.RA)Mathematics::Quantum AlgebraMathematics - Quantum AlgebraFOS: MathematicsQuantum Algebra (math.QA)Mathematics::Symplectic GeometryQuantumMathematical PhysicsCommunications in Algebra
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Moduli spaces of discrete gravity

2003

Spectral triples describe and generalize Riemannian spin geometries by converting the geometrical information into algebraic data, which consist of an algebra $A$, a Hilbert space $H$ carrying a representation of $A$ and the Dirac operator $D$ (a selfadjoint operator acting on $H$). The gravitational action is described by the trace of a suitable function of $D$. In this paper we examine the (path-integral-) quantization of such a system given by a finite dimensional commutative algebra. It is then (in concrete examples) possible to construct the moduli space of the theory, i.e. to divide the space of all Dirac operators by the action of the diffeomorphism group, and to construct an invaria…

PhysicsPure mathematicsGroup (mathematics)Hilbert spaceGeneral Physics and AstronomyObservableSpace (mathematics)Dirac operatorModuli spacesymbols.namesakesymbolsGeometry and TopologyDiffeomorphismInvariant measureMathematical PhysicsJournal of Geometry and Physics
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