中文

The noncommutative Choquet boundary

算子代数 2015-06-26 v4 泛函分析

摘要

Let S be an operator system -- a self-adjoint linear subspace of a unital C*-algebra A such that contains 1 and A=C*(S) is generated by S. A boundary representation for S is an irreducible representation \pi of C*(S) on a Hilbert space with the property that πS\pi\restriction_S has a unique completely positive extension to C*(S). The set S\partial_S of all (unitary equivalence classes of) boundary representations is the noncommutative counterpart of the Choquet boundary of a function system SC(X)S\subseteq C(X) that separates points of X. It is known that the closure of the Choquet boundary of a function system S is the Silov boundary of X relative to S. The corresponding noncommutative problem of whether every operator system has "sufficiently many" boundary representations was formulated in 1969, but has remained unsolved despite progress on related issues. In particular, it was unknown if S\partial_S is nonempty for generic S. In this paper we show that every separable operator system has sufficiently many boundary representations. Our methods use separability in an essential way.

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引用

@article{arxiv.math/0701329,
  title  = {The noncommutative Choquet boundary},
  author = {William Arveson},
  journal= {arXiv preprint arXiv:math/0701329},
  year   = {2015}
}

备注

22 pages. A significant revision, including a new section and many clarifications. No change in the basic mathematics