<p>In this paper, the <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(C^*\)</EquationSource> </InlineEquation>-algebra of the seven-dimensional un-decomposable nilpotent Lie group is characterized explicitly for the first time(see [<CitationRef CitationID="CR8">8</CitationRef>]). Furthermore, the topology of its spectrum is described as a preparation for the analysis of its <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(C^*\)</EquationSource> </InlineEquation>-algebra. Then, the operator-valued Fourier transform is employed to translate the given C*-algebra into the algebra of bounded operator fields through its spectrum. We find the conditions satisfied by the image of the goal to characterize them by these conditions, namely the "norm controlled dual limit" (NCDL)-conditions (see [<CitationRef CitationID="CR14">14</CitationRef>]). The methods used for the nilpotent Lie groups are different for each one. We consider the co-adjoint orbits and, for our case, we use the Kirillov theory.</p>

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Spectrum and fourier analysis of the \(C^*\)-algebra associated with a seven-dimensional nilpotent Lie group

  • Ghofrane Kardi

摘要

In this paper, the \(C^*\) -algebra of the seven-dimensional un-decomposable nilpotent Lie group is characterized explicitly for the first time(see [8]). Furthermore, the topology of its spectrum is described as a preparation for the analysis of its \(C^*\) -algebra. Then, the operator-valued Fourier transform is employed to translate the given C*-algebra into the algebra of bounded operator fields through its spectrum. We find the conditions satisfied by the image of the goal to characterize them by these conditions, namely the "norm controlled dual limit" (NCDL)-conditions (see [14]). The methods used for the nilpotent Lie groups are different for each one. We consider the co-adjoint orbits and, for our case, we use the Kirillov theory.