Let MB(H)M\subseteq B(H) be a with Ω\Omega, and let S=JΔ1/2S=J\Delta^{1/2} be the polar decomposition of its . The natural positive cone is

PΩ={Δ1/4xΩ:xM+}H,P_\Omega^\natural =\overline{\{\Delta^{1/4}x\Omega:x\in M_+\}}\subseteq H,

where the closure is in the Hilbert-space norm, Δ\Delta is the , and JJ is the . Thus PΩP_\Omega^\natural is a distinguished closed convex cone attached to the represented algebra and its modular data, not the operator-positive cone M+M_+. It is the cone used to place this representation in standard form.

Self-duality and invariance

The cone is self-dual:

PΩ={ξH:ξ,η0 for every ηPΩ}.P_\Omega^\natural =\{\xi\in H:\langle\xi,\eta\rangle\geq0 \text{ for every }\eta\in P_\Omega^\natural\}.

It is fixed pointwise by JJ, and xJxJxJxJ maps it into itself for every xMx\in M. These are structural theorems of modular theory, not extra clauses in the displayed construction.

Every on MM is represented by a unique vector ξPΩ\xi\in P_\Omega^\natural through φ(x)=xξ,ξ\varphi(x)=\langle x\xi,\xi\rangle. This uniqueness is one reason the cone is more useful than an arbitrary positive-vector realization.

Relationship to standard form

The quadruple (M,H,J,PΩ)(M,H,J,P_\Omega^\natural) is a of MM. Different cyclic separating vectors may produce different Tomita operators, but the resulting standard forms are canonically unitarily equivalent. Consequently the natural cone expresses positivity in a representation-independent way once the standard-form identification is made.

References
  1. H. Araki, “Some Properties of Modular Conjugation Operator of von Neumann Algebras and a Non-commutative Radon–Nikodym Theorem with a Chain Rule,” Pacific Journal of Mathematics 50 (1974), 309–354. DOI record. Relevant: construction, self-duality, and representation of normal positive functionals by cone vectors.
  2. U. Haagerup, “The Standard Form of von Neumann Algebras,” Mathematica Scandinavica 37 (1975), 271–283. DOI record. Relevant: Theorem 1.6 and Definition 2.1 on the natural cone and standard form.