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modular theory

Context

Physics

physics, mathematical physics

Surveys, textbooks and lecture notes


theory (physics), model (physics)

AQFT and operator algebra

Contents

Idea

This page is about the modular theory introduced by Tomita for von Neumann-algebras. It is important both for the structure theory of von Neumann-algebras and in the Haag-Kastler approach to AQFT, one important example is the Bisognano-Wichmann theorem. It is often called Tomita-Takesaki theory, because the first presentation beyond a preprint is due to Masamichi Takesaki.

Definition

Let be a Hilbert space, a von Neumann-algebra with commutant and a separating and cyclic vector Ω. Then there is a modular operator Δ and a modular conjugation J such that:

  1. Δ is self-adjoint, positive and invertible (but not bounded).

  2. ΔΩ=Ω and JΩ=Ω

  3. J is antilinear, J *=J,J 2=𝟙, J commutes with Δ it. This implies

    Ad(J)Δ=Δ 1Ad(J) \Delta = \Delta^{-1}
  4. For every A the vector AΩ is in the domain of Δ 12 and

    JΔ 12AΩ=A *Ω=:SAΩJ \Delta^{\frac{1}{2}} A \Omega = A^* \Omega =: SA \Omega
  5. The unitary group Δ it defines a group automorphism of :

    Ad(Δ it)=for alltAd(\Delta^{it}) \mathcal{M} = \mathcal{M} \; \; \text{for all} \; t \in \mathbb{R}
  6. J maps to .

References

Many textbooks on operator algebras contain a chapter about modular theory.

MathOverflow question tomita-takesaki-versus-frobenuis-where-is-the-similarity

Revised on March 30, 2013 03:24:09 by Urs Schreiber (89.204.138.192)