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Local nets on Minkowski half-plane associated to lattices Marcel Bischoff Department of Mathematics University of Rome Tor Vergata Bucharest, April 29th, 2011 Marcel Bischoff (Uni Roma II) Local nets on Minkowski half-plane associated


  1. Local nets on Minkowski half-plane associated to lattices Marcel Bischoff Department of Mathematics University of Rome “Tor Vergata” Bucharest, April 29th, 2011 Marcel Bischoff (Uni Roma II) Local nets on Minkowski half-plane associated to lattices Bucharest, April 29th, 2011

  2. Outline Standard subspaces Conformal Nets Nets on Minkowski half-plane Semigroup elements Marcel Bischoff (Uni Roma II) Local nets on Minkowski half-plane associated to lattices Bucharest, April 29th, 2011

  3. Introduction ◮ Algebraic quantum field theory: A family of algebras containing all local observables associated to space-time regions. ◮ Many structural results, recently also construction of interesting models ◮ Conformal field theory (CFT) in 1 and 2 dimension described by AQFT quite successful, e.g. partial classification results (e.g. c < 1 ) (Kawahigashi and Longo, 2004) ◮ Boundary Conformal Quantum Field Theory (BCFT) on Minkowski half-plane: (Longo and Rehren, 2004) ◮ Boundary Quantum Field Theory (BQFT) on Minkowski half-plane: (Longo and Witten, 2010) Marcel Bischoff (Uni Roma II) Local nets on Minkowski half-plane associated to lattices Bucharest, April 29th, 2011

  4. Outline Standard subspaces Conformal Nets Nets on Minkowski half-plane Semigroup elements Marcel Bischoff (Uni Roma II) Local nets on Minkowski half-plane associated to lattices Bucharest, April 29th, 2011

  5. Standard subspaces H complex Hilbert space, H ⊂ H real subspace. Symplectic complement: H ′ = { x ∈ H : Im( x, H ) = 0 } = i H ⊥ Standard subspace: closed, real subspace H ⊂ H with H + i H = H and H ∩ i H = { 0 } . Define antilinear unbounded closed involutive ( S 2 ⊂ 1 ) operator S H : x + i y �→ x − i y for x, y ∈ H. Conversely S densely defined closed, antilinear involution on H , H S = { x ∈ H : Sx = x } is a standard subspace: standard → densely defined, closed, 1:1 ← subspaces H antilinear involutions S Modular Theory: Polar decomposition S H = J H ∆ 1 / 2 H J H H = H ′ ∆ i t H H = H Marcel Bischoff (Uni Roma II) Local nets on Minkowski half-plane associated to lattices Bucharest, April 29th, 2011

  6. Standard subspaces H complex Hilbert space, H ⊂ H real subspace. Symplectic complement: H ′ = { x ∈ H : Im( x, H ) = 0 } = i H ⊥ Standard subspace: closed, real subspace H ⊂ H with H + i H = H and H ∩ i H = { 0 } . Define antilinear unbounded closed involutive ( S 2 ⊂ 1 ) operator S H : x + i y �→ x − i y for x, y ∈ H. Conversely S densely defined closed, antilinear involution on H , H S = { x ∈ H : Sx = x } is a standard subspace: standard → densely defined, closed, 1:1 ← subspaces H antilinear involutions S Modular Theory: Polar decomposition S H = J H ∆ 1 / 2 H J H H = H ′ ∆ i t H H = H Marcel Bischoff (Uni Roma II) Local nets on Minkowski half-plane associated to lattices Bucharest, April 29th, 2011

  7. Standard subspaces H complex Hilbert space, H ⊂ H real subspace. Symplectic complement: H ′ = { x ∈ H : Im( x, H ) = 0 } = i H ⊥ Standard subspace: closed, real subspace H ⊂ H with H + i H = H and H ∩ i H = { 0 } . Define antilinear unbounded closed involutive ( S 2 ⊂ 1 ) operator S H : x + i y �→ x − i y for x, y ∈ H. Conversely S densely defined closed, antilinear involution on H , H S = { x ∈ H : Sx = x } is a standard subspace: standard → densely defined, closed, 1:1 ← subspaces H antilinear involutions S Modular Theory: Polar decomposition S H = J H ∆ 1 / 2 H J H H = H ′ ∆ i t H H = H Marcel Bischoff (Uni Roma II) Local nets on Minkowski half-plane associated to lattices Bucharest, April 29th, 2011

  8. Standard subspaces H complex Hilbert space, H ⊂ H real subspace. Symplectic complement: H ′ = { x ∈ H : Im( x, H ) = 0 } = i H ⊥ Standard subspace: closed, real subspace H ⊂ H with H + i H = H and H ∩ i H = { 0 } . Define antilinear unbounded closed involutive ( S 2 ⊂ 1 ) operator S H : x + i y �→ x − i y for x, y ∈ H. Conversely S densely defined closed, antilinear involution on H , H S = { x ∈ H : Sx = x } is a standard subspace: standard → densely defined, closed, 1:1 ← subspaces H antilinear involutions S Modular Theory: Polar decomposition S H = J H ∆ 1 / 2 H J H H = H ′ ∆ i t H H = H Marcel Bischoff (Uni Roma II) Local nets on Minkowski half-plane associated to lattices Bucharest, April 29th, 2011

  9. Standard subspaces H complex Hilbert space, H ⊂ H real subspace. Symplectic complement: H ′ = { x ∈ H : Im( x, H ) = 0 } = i H ⊥ Standard subspace: closed, real subspace H ⊂ H with H + i H = H and H ∩ i H = { 0 } . Define antilinear unbounded closed involutive ( S 2 ⊂ 1 ) operator S H : x + i y �→ x − i y for x, y ∈ H. Conversely S densely defined closed, antilinear involution on H , H S = { x ∈ H : Sx = x } is a standard subspace: standard → densely defined, closed, 1:1 ← subspaces H antilinear involutions S Modular Theory: Polar decomposition S H = J H ∆ 1 / 2 H J H H = H ′ ∆ i t H H = H Marcel Bischoff (Uni Roma II) Local nets on Minkowski half-plane associated to lattices Bucharest, April 29th, 2011

  10. Standard subspaces and inner functions Standard pair. ( H, T ) ◮ H ⊂ H standard subspace with ◮ T ( t ) = e i tP one-param. group with positive generator P ◮ T ( t ) H ⊂ H for t ≥ 0 Theorem (Borchers Theorem for standard subspaces) Let ( H, T ) be a standard pair, then ∆ i s H T ( t )∆ − i s = T ( e − 2 πs t ) ( s, t ∈ R ) H J H T ( t ) J H = T ( − t ) ( t ∈ R ) Marcel Bischoff (Uni Roma II) Local nets on Minkowski half-plane associated to lattices Bucharest, April 29th, 2011

  11. Standard subspaces and inner functions Standard pair. ( H, T ) ◮ H ⊂ H standard subspace with ◮ T ( t ) = e i tP one-param. group with positive generator P ◮ T ( t ) H ⊂ H for t ≥ 0 Theorem (Borchers Theorem for standard subspaces) Let ( H, T ) be a standard pair, then ∆ i s H T ( t )∆ − i s = T ( e − 2 πs t ) ( s, t ∈ R ) H J H T ( t ) J H = T ( − t ) ( t ∈ R ) Marcel Bischoff (Uni Roma II) Local nets on Minkowski half-plane associated to lattices Bucharest, April 29th, 2011

  12. Standard subspaces and inner functions E ( H ) = unitaries V on H such that V H ⊂ H and [ V, T ( t )] = 0 . Analog of the Beurling-Lax theorem. Characterization of E ( H ) . (Longo and Witten, 2010) ( H, T ) irreducible standard pair, then are equivalent 1. V ∈ E ( H ) , i.e. V H ⊂ H with V unitary on H C commuting with T . R + i R + 2. V = ϕ ( P ) with ϕ boundary value of a symmetric inner analytic L ∞ function ϕ : R + i R + → C , where ◮ symmetric ϕ ( p ) = ϕ ( − p ) for p ≥ 0 ◮ inner | ϕ ( p ) | = 1 for p ∈ R . Marcel Bischoff (Uni Roma II) Local nets on Minkowski half-plane associated to lattices Bucharest, April 29th, 2011

  13. Standard subspaces and inner functions E ( H ) = unitaries V on H such that V H ⊂ H and [ V, T ( t )] = 0 . Analog of the Beurling-Lax theorem. Characterization of E ( H ) . (Longo and Witten, 2010) ( H, T ) irreducible standard pair, then are equivalent 1. V ∈ E ( H ) , i.e. V H ⊂ H with V unitary on H C commuting with T . R + i R + 2. V = ϕ ( P ) with ϕ boundary value of a symmetric inner analytic L ∞ function ϕ : R + i R + → C , where ◮ symmetric ϕ ( p ) = ϕ ( − p ) for p ≥ 0 ◮ inner | ϕ ( p ) | = 1 for p ∈ R . Marcel Bischoff (Uni Roma II) Local nets on Minkowski half-plane associated to lattices Bucharest, April 29th, 2011

  14. Outline Standard subspaces Conformal Nets Nets on Minkowski half-plane Semigroup elements Marcel Bischoff (Uni Roma II) Local nets on Minkowski half-plane associated to lattices Bucharest, April 29th, 2011

  15. Conformal Nets H Hilbert space, I = family of proper intervals on R → A ( I ) = A ( I ) ′′ ⊂ B( H ) I ∋ I �− A. Isotony. I 1 ⊂ I 2 = ⇒ A ( I 1 ) ⊂ A ( I 2 ) B. Locality. I 1 ∩ I 2 = � = ⇒ [ A ( I 1 ) , A ( I 2 )] = { 0 } C. M¨ obius covariance. There is a unitary representation U of the M¨ obius group ( ∼ = PSL(2 , R ) on H such that U ( g ) A ( I ) U ( g ) ∗ = A ( gI ) . D. Positivity of energy. U is a positive-energy representation, i.e. generator L 0 of the rotation subgroup (conformal Hamiltonian) has positive spectrum. E. Vacuum. ker L 0 = C Ω and Ω (vacuum vector) is a unit vector cyclic for the von Neumann algebra � I ∈I A ( I ) . Consequences Complete Rationality Marcel Bischoff (Uni Roma II) Local nets on Minkowski half-plane associated to lattices Bucharest, April 29th, 2011

  16. Net of free bosons. Net of standard subspaces (prequantised theory) �·� using ◮ L R = C ∞ ( S 1 , R ) yields a Hilbert space H = L R ◮ semi-norm. � f � = � k> 0 k | ˆ f k | ◮ complex-structure. J : ˆ → − i sign( k ) ˆ f k �− f k � ◮ symplectic form. ω ( f, g ) = Im( f, g ) = 1 / (4 π ) gd f ◮ Local spaces: L I R = { f L R : supp f ⊂ I } I �− → H ( I ) = L I R ⊂ H Conformal net of a free boson ◮ Second quantization. Conformal net on the symmetric Fock space e H by CCR functor (Weyl unitaries): → A ( I ) := CCR( H ( I )) ′′ ⊂ B( e H ) I �− ◮ Weyl unitaries W ( f ) W ( g ) = e − i ω ( f,g ) W ( f + g ) , ◮ Vacuum state φ ( W ( f )) = (Ω , W ( f )Ω) = e − 1 / 2 � f � 2 Marcel Bischoff (Uni Roma II) Local nets on Minkowski half-plane associated to lattices Bucharest, April 29th, 2011

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