Math 2.0

Functional analysis Definition

Tomita–Takesaki theory

Builds on Von Neumann algebraCommutantHilbert spaceUnbounded operatorUnitary operator

Definition

Let MM be a von Neumann algebra on a complex Hilbert space HH, with commutant M′M'. Let Ω∈H\Omega \in H be cyclic for MM, that is, MΩM\Omega is dense in HH. Assume also that Ω\Omega is separating for MM: if x∈Mx \in M and xΩ=0x\Omega = 0, then x=0x = 0.

  1. The operator S0S_0 with domain MΩM\Omega defined by S0(xΩ)=x∗ΩS_0(x\Omega) = x^*\Omega is a well-defined, densely defined, closable antilinear unbounded operator; let SS be its closure.
  2. The modular operator is the positive self-adjoint operator Δ=S∗S\Delta = S^* S, and the modular conjugation is the antiunitary operator JJ in the polar decomposition S=JΔ1/2S = J \Delta^{1/2}.
  3. The modular automorphism group is σt(x)=ΔitxΔ−it\sigma_t(x) = \Delta^{it} x \Delta^{-it} for t∈ℝt \in \R and x∈Mx \in M.

Tomita–Takesaki theory is the study of these objects. Its main theorem states that JMJ=M′J M J = M' and ΔitMΔ−it=M\Delta^{it} M \Delta^{-it} = M for all t∈ℝt \in \R. So each σt\sigma_t is an automorphism of MM.

Remarks

Example: let M=Mn(ℂ)M = M_n(\C) act by left multiplication on H=Mn(ℂ)H = M_n(\C) with inner product ⟨ξ,η⟩=tr⁡(η∗ξ)\langle \xi, \eta \rangle = \operatorname{tr}(\eta^* \xi), and let Ω=ρ1/2\Omega = \rho^{1/2} for an invertible density matrix ρ\rho. Then Ω\Omega is cyclic and separating, Δξ=ρξρ−1\Delta \xi = \rho \xi \rho^{-1} and Jξ=ξ∗J \xi = \xi^*. Check: JΔ1/2(xρ1/2)=J(ρ1/2x)=x∗ρ1/2=S(xρ1/2)J \Delta^{1/2}(x \rho^{1/2}) = J(\rho^{1/2} x) = x^* \rho^{1/2} = S(x\rho^{1/2}). Here JMJJMJ is the algebra of right multiplications, which is M′M', and σt(x)=ρitxρ−it\sigma_t(x) = \rho^{it} x \rho^{-it}.

Non-example: let M=B(H)M = B(H) with dim⁡H≥2\dim H \ge 2, let Ω\Omega be a unit vector, and let η\eta be a unit vector orthogonal to Ω\Omega. Every nonzero vector is cyclic for B(H)B(H), but Ω\Omega is not separating. Indeed, the operator x=⟨⋅,η⟩Ωx = \langle \cdot, \eta \rangle \Omega is nonzero and xΩ=0x\Omega = 0. Its adjoint is x∗=⟨⋅,Ω⟩ηx^* = \langle \cdot, \Omega \rangle \eta, so x∗Ω=η≠0x^*\Omega = \eta \ne 0. Since xΩ=0Ωx\Omega = 0\Omega but x∗Ω≠0∗Ωx^*\Omega \ne 0^*\Omega, the formula for S0S_0 does not define a map.

The vector state φ(x)=⟨xΩ,Ω⟩\varphi(x) = \langle x\Omega, \Omega \rangle is a KMS state for the modular automorphism group, and Takesaki showed that σ\sigma is the only one-parameter automorphism group of MM with this property.

Reading path

To understand this page from the ground up, read these 6 pages in order. The foundations come first.

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Each page uses the pages above it. The colour of the bar on a box shows how strong the evidence is, and the box also gives it as text. The list has the same pages.
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  1. Commutant concept
  2. Hilbert space concept
  3. Unbounded operator concept
  4. Unitary operator concept
  5. Von Neumann algebra concept
  6. Tomita–Takesaki theory definition

Further reading

  1. Web https://en.wikipedia.org/wiki/Tomita–Takesaki_theory
About this page
TagRMEF8T6C0E
URIm2://RMEF8T6C0E
Kinddefinition
WritingW0 stub
MSC46L10, 46L40
DefinesTomita–Takesaki theory
UsesVon Neumann algebra, Commutant, Hilbert space, Unbounded operator, Unitary operator
Changed2 November 2026

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