Let M⊆B(H)M\subseteq B(H) be a and let Ω∈H\Omega\in H be both a and a for MM. On the dense subspace MΩM\Omega, define the antilinear operator

S0(xΩ)=x∗Ω,x∈M.S_0(x\Omega)=x^*\Omega,\qquad x\in M.

Separatingness makes this formula well-defined, and cyclicity makes its domain dense. The operator S0S_0 is closable; its closure S=S0‾S=\overline{S_0} is the Tomita operator of (M,Ω)(M,\Omega). It is closed, densely defined, and satisfies S2ξ=ξS^2\xi=\xi whenever both sides are defined.

Closability and the commutant

The companion operator F0(x′Ω)=x′∗ΩF_0(x'\Omega)=x'^*\Omega on M′ΩM'\Omega is densely defined because separatingness for MM is equivalent to cyclicity for the M′M'. The inclusions S0∗⊇F0S_0^*\supseteq F_0 and F0∗⊇S0F_0^*\supseteq S_0 prove that both operators are closable. In fact, their closures satisfy S∗=FS^*=F.

Polar decomposition and modular data

The of the closed antilinear operator is

S=JΔ1/2.S=J\Delta^{1/2}.

Here JJ is the and Δ=S∗S\Delta=S^*S is the . These objects depend on the pair (M,Ω)(M,\Omega), not on MM alone. Their decisive properties are the content of the .

Examples and scope

For M=B(K)M=B(K) acting by left multiplication on the HS⁡(K)\operatorname{HS}(K), the identity Hilbert–Schmidt vector is available only when KK is finite-dimensional; then S(x)=x∗S(x)=x^*. More generally a faithful supplies a cyclic separating vector in the standard Hilbert–Schmidt realization.

References
  1. Masamichi Takesaki, Theory of Operator Algebras I, Springer, 1979. DOI record. Relevant: Chapter VI, §1 on the closable operators S0S_0 and F0F_0.