Báo cáo toán học: " The Embedding of Haagerup Lop Spaces" doc

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Báo cáo toán học: " The Embedding of Haagerup Lop Spaces" doc

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Vietnam Journal of Mathematics 34:3 (2006) 353–356 The Embedding of Haagerup L p Spaces Phan Viet Thu Faculty of Math., Mech. and Inform., Hanoi University of Science 334 Nguyen Trai, Thanh Xuan, Hanoi, Vietnam Received April 18, 2006 Abstract. The aim of this pap er is to give a proof for a theorem due to S. Goldstein that: If there is a σ- weakly continuous faithful projection of norm one from a von Neumann algebra M onto its von Neumann subalgebra N , then L p (N ) can be canon- ically embeded into L p (M ). Here L p (A) [6] denotes the Haagerup L p space over the von Neumann algebra A. 2000 Mathematics Subject Classification: 46L52, 81R15. Keywords: von Neumann algebras, Haagerup spaces, conditional expection for von Neumann algebras. Let M be a von Neumann algebra acting in a Hilbert space H and ψ a normal faithful semifinite weight on M . Let {σ ψ t } t∈R denote the modular automorphism group on M associated with ψ. The crossed pro duct M = M  σ t R is a von Neumann algebra acting on H = L 2 (R,H) generated by (π M (a)ξ)(t)=σ ψ −t (a)ξ(t), (λ M (s)ξ)(t)=ξ(t − s) ξ ∈ H,t ∈ R. (1) Theorem. Let N be a von Neumann subalgebra of M. Suppose that ψ|N is semifinite and σ ψ t |N = σ ψ|N t for each t ∈ R. Then N, the crossed product of N , is canonically embeded into M and for each p ∈ [1, ∞] the space L p (N ) can be canonically embeded into L p (M ), so that for any k ∈ L p (N ) k N p = k M p , where . N p and . M p denote the norms of L p (N ) and L p (M ) respectively. 354 Phan Viet Thu Proof. The condition σ ψ t | N = σ ψ|N t means that ∀b ∈ N , σ ψ t (b)=σ ψ|N t (b) ∈ N , i.e. σ φ t leaves N invariant; Together with the condition that ψ|N is semifinite, it implies, by a theorem of Takesaki [5], that there is a σ-weakly continuous projection E of norm one of M onto N such that ψ =(ψ| N ) ◦ E. It is not hard to show that E ◦ σ ψ = σ ψ ◦ E (see for example, [4, Proposition 3.2]). Let N = N  σ ψ|N t R, it is a von Neumann algebra acting on L 2 (R,H)=H, generated by operators π N (b),b∈ N and λ N (s),s ∈ R; defined by (π( b)ξ(t)=σ ψ|N −t (b)ξ(t)), (λ(s)ξ(t)=ξ(t − s)) ξ ∈ H,t ∈ R. (2) Sine σ ψ|N −t (b)=(σ ψ −t |N )(b) for b ∈ N ; (1) and (2) imply π M |N = π N , (3) λ M = λ N , and M, N act on the same Hilbert space H. Let M 0 be the * algebra generated algebraically by operators π M (a), a ∈ M and λ M (s),s ∈ R. Then M is the σ-weak closure of M 0 and any element x 0 ∈ M 0 can be represented as x 0 = n  k=1 λ M (s k )π M (a k ) for some {s k } n 1 ⊂ R; {a k } n 1 ⊂ M. We define N 0 in the same way. Thus ∀y 0 ∈ N 0 , y 0 = m  k=1 λ N (s k )π N (b k )= m  k=1 λ M (s k )(π M |N )(b k ) ∈ M 0 for some {s k } m 1 ⊂ R; {b k } m 1 ⊂ N . The σ-weak closure of N 0 is N. Then we have N 0 ⊂ M 0 and their σ-weak closures verify N ⊂ M. It is clear that ∀x ∈ N ⊂ M; ||x|| (N) = ||x|| (M) . Consider now the dual action θ s of R in M, characterized by θ s (π M (a)) = π M (a), ∀a ∈ M, θ s (λ M (t)) = e −ist λ M (t), ∀t, s ∈ R. (4) By (3), we have θ s (π N (a)) = π N (a), ∀a ∈ N, θ s (λ N (t)) = e −ist λ N (t), ∀t, s ∈ R. Thus θ s (y 0 ) ∈ N 0 for y 0 ∈ N 0 , ∀s ∈ R. So that θ s (N 0 ) ⊂ N 0 ⊂ N. Since θ s is σ-weakly continuous on M; for all s ∈ R we have θ s (N) ⊂ N. The continuity of θ s in measure implies also The Embedding of Haagerup L p Spaces 355 θ s (  N) ⊂  N and θ M s | N = θ N s , ∀s ∈ R, where θ M s and θ N s denote the dual action θ s of R on M and on N respectively. By definition of L p (N ) and L p (M ) and the above results, it follows that L p (N )={k ∈  N|∀s ∈ R : θ N s k = e − s p k} (5) = {k ∈  N ⊂  M|∀s ∈ R : θ M s k = e − s p k}⊂L p (M ). Then we have L p (N ) ⊂ L p (M ). It remains now to show that k M p = k N p for any k ∈ L p (N ) ⊂ L p (M ). It suffices to demonstrate it for the case p = 1. Note that L 1 (M )  M ∗ ; L 1 (N )  N ∗ and for any φ ∈ N ∗ ; φ ◦ E ∈ M ∗ . In [1, 2] the author has proved that E can be extended canonically to ˆ E : M ∧ + → N ∧ + ;  E :  M →  N and E 1 : L 1 (M ) → L 1 (N ), given by h (φ) → h φ◦E . It is extended also to E p : L p (M ) → L p (N ); and for any φ ∈ N ∗ φ =(φ ◦ E) − | N . Let us calculate the norm of h N φ = h M φ◦E . Note that ||h N φ || (N) 1 = ||φ|| (N) and ||h M φ◦E || (M) 1 = ||φ ◦ E|| (M) for any φ ∈ N ∗ . We have φ (N) = sup b∈N,b≤1 |φ(b)|≥ sup a∈M,a≤1 |(φ ◦ E)(a)| = φ ◦ E (M) ≥ sup b∈N,b≤1 |(φ ◦ E)(b)| = sup b∈N,b≤1 |φ(b)| = φ (N) . (6) This implies φ (N) = φ ◦ E (M) ; i.e. h N φ  (N) 1 = h M φ◦E  (M) 1 , which shows that for any k ∈ L 1 (N ) ⊂ L 1 (M ), one has k (N) 1 = k (M) 1 . It is now obvious that, for each p ∈ [1, ∞], k (N) p = k (M) p , ∀k ∈ L p (N ) ⊂ L p (M ). References 1. S. Goldstein, Conditional expectations and Stochastic integrals in non commu- tative L p -spaces, Math. Proc. Camb. Phil. Soc. 110 (1991) 365–383. 2. S. Goldstein, Norm convergence of martingales in L p -spaces over von Neumann algebras, Revue Roumaine de Math. Pures et Appl. 32 (1987) 531–541. 3. R. V. Kadison and J. R. Ringrose, Fundamentals of the Theory of Operator Alge- bras, Vol.I, 1983; Vol.II, 1986. Academic Press, New York – London. 4. C. E. Lance, Martingale convergence in von Neumann algebras, Math. Proc. Camb. Phil. Soc. 84 (1978) 47–56. 356 Phan Viet Thu 5. M. Takesaki, Conditional expectations in von Neumann algebras, J. Funct. Anal. 9 (1972) 306–321. 6. M. Terp, L p -spaces Associated with von Neumann Algebras, Notes Kφbenhavns Universitet, Matematisk Institut, N 0 . 3, 1981. . Vietnam Journal of Mathematics 34:3 (2006) 353–356 The Embedding of Haagerup L p Spaces Phan Viet Thu Faculty of Math., Mech. and Inform., Hanoi University of Science 334 Nguyen Trai,. N. The continuity of θ s in measure implies also The Embedding of Haagerup L p Spaces 355 θ s (  N) ⊂  N and θ M s | N = θ N s , ∀s ∈ R, where θ M s and θ N s denote the dual action θ s of. Vietnam Received April 18, 2006 Abstract. The aim of this pap er is to give a proof for a theorem due to S. Goldstein that: If there is a σ- weakly continuous faithful projection of norm one from a von Neumann

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