Let AA be a and let φ\varphi be a on AA. The GNS construction associates a HφH_\varphi, a *-representation πφ:AB(Hφ)\pi_\varphi:A\to B(H_\varphi), and a vector ξφ\xi_\varphi such that

φ(a)=πφ(a)ξφ,ξφ(aA)\varphi(a)=\langle\pi_\varphi(a)\xi_\varphi,\xi_\varphi\rangle \quad(a\in A)

and πφ(A)ξφ\pi_\varphi(A)\xi_\varphi is dense in HφH_\varphi.

Cyclicity and assumptions

The triple (πφ,Hφ,ξφ)(\pi_\varphi,H_\varphi,\xi_\varphi) is a . The functional is bounded automatically; neither unitality of AA nor faithfulness of φ\varphi is assumed.

Quotient construction

Set Nφ={aA:φ(aa)=0}N_\varphi=\{a\in A:\varphi(a^*a)=0\}. The formula

[a],[b]φ=φ(ba)\langle[a],[b]\rangle_\varphi=\varphi(b^*a)

defines an , linear in the first variable, on A/NφA/N_\varphi. Completing gives HφH_\varphi, and left multiplication gives πφ(a)[b]=[ab]\pi_\varphi(a)[b]=[ab]. If AA is unital, then ξφ=[1]\xi_\varphi=[1]. In the nonunital case, the bounded extension of φ\varphi to the , or equivalently an , produces the canonical .

Example: evaluation on continuous functions

Take A=C(X)A=C(X) for a compact Hausdorff space XX, choose x0Xx_0\in X, and let φ(f)=f(x0)\varphi(f)=f(x_0). This is a positive functional. With the convention that inner products are linear in the first variable,

[f],[g]φ=φ(gf)=f(x0)g(x0).\langle[f],[g]\rangle_\varphi =\varphi(\overline g f) =f(x_0)\,\overline{g(x_0)}.

Here Nφ={f:f(x0)=0}N_\varphi=\{f:f(x_0)=0\}, so the quotient is one-dimensional and [f]f(x0)[f]\mapsto f(x_0) identifies HφH_\varphi with C\mathbb C. The cyclic vector is [1][1], and

πφ(h)z=h(x0)z,πφ(h)[1]=[h],πφ(h)[1],[1]=h(x0)=φ(h).\begin{aligned} \pi_\varphi(h)z&=h(x_0)z,\\ \pi_\varphi(h)[1]&=[h],\\ \langle\pi_\varphi(h)[1],[1]\rangle&=h(x_0)=\varphi(h). \end{aligned}

The example makes the quotient concrete: functions indistinguishable at x0x_0 become the same vector, and the representation remembers only their value there.

Uniqueness and faithfulness

If (π,H,ξ)(\pi,H,\xi) is another cyclic realization of φ\varphi, the rule πφ(a)ξφπ(a)ξ\pi_\varphi(a)\xi_\varphi\mapsto\pi(a)\xi extends to a unitary intertwining the two representations and carrying ξφ\xi_\varphi to ξ\xi. Hence the pointed cyclic representation is unique up to a unique unitary of this form. The representation πφ\pi_\varphi need not be faithful: its kernel consists of those elements acting trivially on the quotient, a stronger condition than merely belonging to NφN_\varphi.

States and von Neumann algebras

The zero functional gives the zero Hilbert space and the zero representation; the zero vector is cyclic there. This edge case is included by the definition, although states are usually used when a nonzero cyclic vector is desired.

When AA is unital, ξφ2=φ(1)=φ\|\xi_\varphi\|^2=\varphi(1)=\|\varphi\|; in particular a state gives a unit cyclic vector. If A=MA=M is a and φ\varphi is normal, then πφ\pi_\varphi is a . GNS also extends to suitable densely defined weights, but the construction then starts from the left ideal of square-integrable elements rather than all of MM; that extension is not part of the bounded-functional definition above.

References
  1. Gerard J. Murphy, CC^*-Algebras and Operator Theory, Academic Press, 1990. DOI record. Relevant: §3.3 on the GNS construction and cyclic representations.
  2. Gert K. Pedersen, CC^*-Algebras and Their Automorphism Groups, 2nd ed., Academic Press, 2018. DOI record. Relevant: §3.3 on positive functionals and representations.