Associative Algebra

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Paul S Pedersen - One of the best experts on this subject based on the ideXlab platform.

  • cauchy s integral theorem on a finitely generated real commutative and Associative Algebra
    Advances in Mathematics, 1997
    Co-Authors: Paul S Pedersen
    Abstract:

    LetR[α]=R[α1, α2, …, αn] (whereα1=1) be a real, unitary, finitely generated, commutative, and Associative Algebra. We consider functionsf(z)=f(∑ni=1 xiαi) which mapR[α]n={∑ni=1 aiαi | 1⩽i⩽n,ai∈R} intoR[α]=finite dimensional subspaces of {∑k∈Nn0 bkαk | bk∈R,k=(k1, …, kn)∈Nn0} whereN0={0, 1, 2, …}. We impose a total order on an algorithmically defined basisBforR[α]. The resulting Algebra and ordered basis will be written as (R[α], <). We then use this basis to define a norm ‖·‖ on (R[α], <). Continuous functions, differentiable functions, and the concept of Riemann integration will then be defined and discussed in this new setting. We then show that ∫γ f(z) dz=0 whenf(z) is a continuous and differentiable function defined in a simply connected regionG⊂R[α]n⊂(R[α], <) containing the closed pathγ.

Franklin E Schroeck - One of the best experts on this subject based on the ideXlab platform.

  • the poincare group in a demisemidirect product with a non Associative Algebra with representations that include particles and quarks ii
    International Journal of Theoretical Physics, 2009
    Co-Authors: Franklin E Schroeck
    Abstract:

    The quarks and particles’ mass and mass/spin relations are provided with coordinates in configuration space and/or momentum space by means of the marriage of ordinary Poincare group representations with a non-Associative Algebra made through a demisemidirect product, in the notation of Leibniz Algebras. Thus, we circumvent the restriction that the Poincare group cannot be extended to a larger group by any means (including the (semi)direct product) to get even the mass relations. Finally, we will discuss a connection between the phase space representations of the Poincare group and the phase space representations of the associated Leibniz Algebra.

  • the poincaŕ group in a demisemidirect product with a non Associative Algebra with representations that include particles and quarks
    GEOMETRIC METHODS IN PHYSICS, 2008
    Co-Authors: Franklin E Schroeck
    Abstract:

    The quarks have always been a puzzle, as have the particles’ mass and mass/spin relations as they seemed to have no coordinates in configuration space and/or momentum space. The solution to this seems to lie in the marriage of ordinary Poincare group representations with a non‐Associative Algebra made through a demisemidirect product. Then, the work of G. Dixon applies; so, we may obtain all the relations between masses, mass and spin, and the attribution of position and momentum to quarks—this in spite of the old restriction that the Poincare group cannot be extended to a larger group by any means (including the (semi)direct product) to get even the mass relations. Finally, we will briefly discuss a possible connection between the phase space representations of the Poincare group and the phase space representations of the object we will obtain. This will take us into Leibniz (co)homology.

Apurba Das - One of the best experts on this subject based on the ideXlab platform.

Luca Vitagliano - One of the best experts on this subject based on the ideXlab platform.

  • on the strong homotopy Associative Algebra of a foliation
    Communications in Contemporary Mathematics, 2015
    Co-Authors: Luca Vitagliano
    Abstract:

    An involutive distribution C on a smooth manifold M is a Lie-algebroid acting on sections of the normal bundle TM/C. It is known that the Chevalley–Eilenberg complex associated to this representation of C possesses the structure 𝕏 of a strong homotopy Lie–Rinehart Algebra. It is natural to interpret 𝕏 as the (derived) Lie–Rinehart Algebra of vector fields on the space P of integral manifolds of C. In this paper, we show that 𝕏 is embedded in an A∞-Algebra 𝔻 of (normal) differential operators. It is natural to interpret 𝔻 as the (derived) Associative Algebra of differential operators on P. Finally, we speculate about the interpretation of 𝔻 as the universal enveloping strong homotopy Algebra of 𝕏.

  • on the strong homotopy Associative Algebra of a foliation
    arXiv: Differential Geometry, 2012
    Co-Authors: Luca Vitagliano
    Abstract:

    An involutive distribution $C$ on a smooth manifold $M$ is a Lie-algebroid acting on sections of the normal bundle $TM/C$. It is known that the Chevalley-Eilenberg complex associated to this representation of $C$ possesses the structure $\mathbb{X}$ of a strong homotopy Lie-Rinehart Algebra. It is natural to interpret $\mathbb{X}$ as the (derived) Lie-Rinehart Algebra of vector fields on the space $\mathbb{P}$ of integral manifolds of $C$. In this paper, I show that $\mathbb{X}$ is embedded in a strong homotopy Associative Algebra $\mathbb{D}$ of (normal) differential operators. It is natural to interpret $\mathbb{D}$ as the (derived) Associative Algebra of differential operators on $\mathbb{P}$. Finally, I speculate about the interpretation of $\mathbb{D}$ as the universal enveloping strong homotopy Algebra of $\mathbb{X}$.

A. Berzins - One of the best experts on this subject based on the ideXlab platform.