Definition

Let AA be a nonzero . For every φS(A)\varphi\in S(A), choose its (πφ,Hφ,ξφ)(\pi_\varphi,H_\varphi,\xi_\varphi). The universal representation is the

πu=φS(A)πφonHu=φS(A)Hφ.\pi_u=\bigoplus_{\varphi\in S(A)}\pi_\varphi \quad\text{on}\quad H_u=\bigoplus_{\varphi\in S(A)}H_\varphi.

It is a faithful . Its unitary-equivalence class does not depend on the chosen models of the GNS triples. “Universal” here refers to simultaneously containing the cyclic representations generated by states, not to an initial or among all representations.

Why it is faithful

States separate the positive elements of a CC^*-algebra: for every nonzero aa, some state is nonzero on aaa^*a. The corresponding GNS summand then acts nontrivially on aa, so πu(a)0\pi_u(a)\neq0. This also gives a direct GNS proof of the faithful-representation part of the Murphy, §§3.3–3.4.

Enveloping von Neumann algebra

The πu(A)\pi_u(A)'' is canonically isomorphic, as a , to the bidual AA^{**}. Under this identification the canonical map AAA\to A^{**} agrees with πu\pi_u, and every bounded functional on AA extends uniquely to a on AA^{**}. This is the universal enveloping von Neumann algebra construction Takesaki, vol. I, Chapter III.

Scope of the sum

Some sources sum GNS representations over all , or choose only enough states to separate points. Such sums can also be faithful, but their multiplicities—and even their unitary-equivalence classes—need not agree with πu\pi_u. The definition here fixes the direct sum over all states. It should not be confused with a universal CC^*-algebra specified by generators and relations.

References
  1. Gerard J. Murphy, C-Algebras and Operator Theory*, Academic Press, 1990. DOI record. Relevant: §§3.3–3.4 on GNS representations and the faithful representation theorem.
  2. Masamichi Takesaki, Theory of Operator Algebras I, Springer, 1979. DOI record. Relevant: Chapter III on the universal representation and enveloping von Neumann algebra.