English

The noncommutative Choquet boundary

Operator Algebras 2015-06-26 v4 Functional Analysis

Abstract

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.

Keywords

Cite

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

Comments

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