On the Characterization of Trace Class Representations and Schwartz Operators
Journal of Lie Theory, Volume 26 (2016) no. 3, pp. 787-805
\def\cH{{\cal H}} We collect several characterizations of unitary representations $(\pi, \cH)$ of a finite dimensional Lie group $G$ which are trace class, i.e., for each compactly supported smooth function $f$ on $G$, the operator $\pi(f)$ is trace class. In particular we derive the new result that, for some $m \in \mathbb{N}$, all operators $\pi(f)$, $f \in C^m_c(G)$, are trace class. As a consequence the corresponding distribution character $\theta_\pi$ is of finite order. We further show $\pi$ is trace class if and only if every operator $A$, which is smoothing in the sense that $A\cH\subseteq \cH^\infty$, is trace class and that this in turn is equivalent to the Fr\'echet space $\cH^\infty$ being nuclear, which in turn is equivalent to the realizability of the Gaussian measure of $\cH$ on the space $\cH^{-\infty}$ of distribution vectors. Finally we show that, even for infinite dimensional Fr\'echet-Lie groups, $A$ and $A^*$ are smoothing if and only if $A$ is a Schwartz operator, i.e., all products of $A$ with operators from the derived representation are bounded.
DOI: 10.5802/jolt.913
Classification: 22E45, 22E66
Keywords: Trace class representation, smoothing operator, Schwartz operator, unitary representation
@article{JOLT_2016_26_3_a11,
     author = {G. van Dijk and K.-H. Neeb and H. Salmasian and C. Zellner},
     title = {On the {Characterization} of {Trace} {Class} {Representations} and {Schwartz} {Operators}},
     journal = {Journal of Lie Theory},
     pages = {787--805},
     year = {2016},
     volume = {26},
     number = {3},
     doi = {10.5802/jolt.913},
     zbl = {1348.22017},
     url = {https://jolt.centre-mersenne.org/articles/10.5802/jolt.913/}
}
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G. van Dijk; K.-H. Neeb; H. Salmasian; C. Zellner. On the Characterization of Trace Class Representations and Schwartz Operators. Journal of Lie Theory, Volume 26 (2016) no. 3, pp. 787-805. doi: 10.5802/jolt.913

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