Definition

Let π:AB(H)\pi:A\to B(H) be a . A vector ξH\xi\in H is cyclic for π\pi when

span{π(a)ξ:aA}=H.\overline{\operatorname{span}}\{\pi(a)\xi:a\in A\}=H.

The representation is cyclic if it has at least one . For a nonunital algebra the closure in this formula is essential. The existence of a cyclic vector forces π\pi to be nondegenerate: the closed span of π(A)H\pi(A)H is then all of HH. Cyclicity is a property of the represented action together with its , not merely of AA.

Equivalent viewpoint

A vector is cyclic for π(A)\pi(A) if and only if it is separating for the π(A)\pi(A)': an operator Tπ(A)T\in\pi(A)' satisfying Tξ=0T\xi=0 must be zero. This converts density of one orbit into uniqueness detected by the commuting operators.

Sources of cyclic representations

The associated with a produces a cyclic representation whose distinguished cyclic vector recovers the functional as a vector functional. Conversely, every cyclic representation with a chosen unit cyclic vector yields a state aπ(a)ξ,ξa\mapsto\langle\pi(a)\xi,\xi\rangle. This correspondence is treated in Murphy, section 3.3.

Examples and limits

The identity representation of C(X)C(X) on L2(X,μ)L^2(X,\mu) is cyclic when the constant function 11 belongs to the space and bounded continuous functions are dense there. A direct sum of cyclic representations need not be cyclic: one vector must simultaneously generate every summand with enough independence.

References
  1. Gerald J. Murphy, CC^*-Algebras and Operator Theory, Academic Press, 1990. Publisher record. Relevant: section 3.3 on cyclic representations and the GNS construction.