Orthomodular lattices, natural density and non-distributive Lp spaces Relations Between Banach Space Theory and Geometric Measure Theory Jarno Talponen University of Eastern Finland talponen@iki.fi June, 2015 Jarno Talponen (UEF) On generalized measure algebras June, 2015 1 / 12 Abstract The undercurrent in the paper involves orthomodular lattices and generalized measure algebras where one replaces Boolean algebra & a measure with a lattice & a submeasure. In the first part of the talk we take a look at natural density of natural numbers and how it can be related to measure algebras. The second part of the paper and talk are speculative in nature. We discuss how Lp spaces on lattices with submeasures ‘should’ look like. Then the ‘supports’ of simple functions do not behave distributively as in the Boolean case. The preprint is available at ArXiv. Jarno Talponen (UEF) On generalized measure algebras June, 2015 2 / 12 Lattice Lattice L = (L, ∨, ∧, 0, 1) is axiomatized quite similarly as a Boolean algebra. Typically Boolean algebras and lattices differ in complementation and distributivity; the latter does not need to enjoy such properties. Jarno Talponen (UEF) On generalized measure algebras June, 2015 3 / 12 Lattice Lattice L = (L, ∨, ∧, 0, 1) is axiomatized quite similarly as a Boolean algebra. Typically Boolean algebras and lattices differ in complementation and distributivity; the latter does not need to enjoy such properties. However, a lattice may have weaker versions of complementation operation A 7→ A⊥ and that of distributivity. An example of such a structure: orthomodular lattice. Jarno Talponen (UEF) On generalized measure algebras June, 2015 3 / 12 Lattice Lattice L = (L, ∨, ∧, 0, 1) is axiomatized quite similarly as a Boolean algebra. Typically Boolean algebras and lattices differ in complementation and distributivity; the latter does not need to enjoy such properties. However, a lattice may have weaker versions of complementation operation A 7→ A⊥ and that of distributivity. An example of such a structure: orthomodular lattice. A model for such a lattice: the system of closed subspaces of a Hilbert space. Jarno Talponen (UEF) On generalized measure algebras June, 2015 3 / 12 Lattice Lattice L = (L, ∨, ∧, 0, 1) is axiomatized quite similarly as a Boolean algebra. Typically Boolean algebras and lattices differ in complementation and distributivity; the latter does not need to enjoy such properties. However, a lattice may have weaker versions of complementation operation A 7→ A⊥ and that of distributivity. An example of such a structure: orthomodular lattice. A model for such a lattice: the system of closed subspaces of a Hilbert space. A generalization of measure: An order-preserving map ϕ : L → [0, 1] with ϕ(0) = 0, ϕ(1) = 1, ϕ(A ∨ B) ≤ ϕ(A) + ϕ(B), A, B ∈ L is called a submeasure. Jarno Talponen (UEF) On generalized measure algebras June, 2015 3 / 12 Lattice Lattice L = (L, ∨, ∧, 0, 1) is axiomatized quite similarly as a Boolean algebra. Typically Boolean algebras and lattices differ in complementation and distributivity; the latter does not need to enjoy such properties. However, a lattice may have weaker versions of complementation operation A 7→ A⊥ and that of distributivity. An example of such a structure: orthomodular lattice. A model for such a lattice: the system of closed subspaces of a Hilbert space. A generalization of measure: An order-preserving map ϕ : L → [0, 1] with ϕ(0) = 0, ϕ(1) = 1, ϕ(A ∨ B) ≤ ϕ(A) + ϕ(B), A, B ∈ L is called a submeasure. Relevance: Quantum theory. Jarno Talponen (UEF) On generalized measure algebras June, 2015 3 / 12 Natural density sets Let us denote by D the collection of all density sets, i.e. sets A ⊂ N such that the natural density |A ∩ {1, . . . , n}| n→∞ n d(A) := lim exists. We denote by N ⊂ D the collection of all null density sets, i.e. sets A with d(A) = 0. Equivalence relation: A ∼ B if A M B ∈ N . Jarno Talponen (UEF) On generalized measure algebras June, 2015 4 / 12 Natural density sets Let us denote by D the collection of all density sets, i.e. sets A ⊂ N such that the natural density |A ∩ {1, . . . , n}| n→∞ n d(A) := lim exists. We denote by N ⊂ D the collection of all null density sets, i.e. sets A with d(A) = 0. Equivalence relation: A ∼ B if A M B ∈ N . Important in number theory. Have been studied in Banach spaces too. Jarno Talponen (UEF) On generalized measure algebras June, 2015 4 / 12 Natural density sets Let us denote by D the collection of all density sets, i.e. sets A ⊂ N such that the natural density |A ∩ {1, . . . , n}| n→∞ n d(A) := lim exists. We denote by N ⊂ D the collection of all null density sets, i.e. sets A with d(A) = 0. Equivalence relation: A ∼ B if A M B ∈ N . Important in number theory. Have been studied in Banach spaces too. Notoriously badly behaved: A ∩ B, A ∪ B may fail to be density sets even if A and B are such. Jarno Talponen (UEF) On generalized measure algebras June, 2015 4 / 12 Natural density sets Let us denote by D the collection of all density sets, i.e. sets A ⊂ N such that the natural density |A ∩ {1, . . . , n}| n→∞ n d(A) := lim exists. We denote by N ⊂ D the collection of all null density sets, i.e. sets A with d(A) = 0. Equivalence relation: A ∼ B if A M B ∈ N . Important in number theory. Have been studied in Banach spaces too. Notoriously badly behaved: A ∩ B, A ∪ B may fail to be density sets even if A and B are such. Singletons have density 0, thus σ-additivity of d fails. Jarno Talponen (UEF) On generalized measure algebras June, 2015 4 / 12 A result on turning a system of density sets to a measure algebra But if the previous obstructions are dealt with, then the measure sets turn to measure algebras. Jarno Talponen (UEF) On generalized measure algebras June, 2015 5 / 12 A result on turning a system of density sets to a measure algebra But if the previous obstructions are dealt with, then the measure sets turn to measure algebras. Jarno Talponen (UEF) On generalized measure algebras June, 2015 5 / 12 A result on turning a system of density sets to a measure algebra But if the previous obstructions are dealt with, then the measure sets turn to measure algebras. Theorem Let F ⊂ D be a family closed under finite intersections. Then there is a σ-algebra Σ order-isomorphically included in D/∼ such that F/∼ ⊂ Σ and d̂ : Σ → [0, 1], d̂(K /∼ ) = d(K ), is σ-additive. Morerover, if F/∼ is countable and the corresponding σ-generated measure algebra (Σ, d̂) is atomless, then it is in fact isomorphic to the measure algebra on the unit interval. Jarno Talponen (UEF) On generalized measure algebras June, 2015 5 / 12 Structure of the proof 1/2: σ-additivity of d on the cosets Jarno Talponen (UEF) On generalized measure algebras June, 2015 6 / 12 Structure of the proof 1/2: σ-additivity of d on the cosets Lemma With the above notations the mapping d̂ is countably additive in the following sense: Suppose that ([Ak ])k∈N ⊂ D/ -increasing W W∼ is a N W sequence. Then k [Ak ] ∈ D/∼ exists and d̂( k [Ak ]) = k d̂([Ak ]). Jarno Talponen (UEF) On generalized measure algebras June, 2015 6 / 12 Structure of the proof 1/2: σ-additivity of d on the cosets Lemma With the above notations the mapping d̂ is countably additive in the following sense: Suppose that ([Ak ])k∈N ⊂ D/ -increasing W W∼ is a N W sequence. Then k [Ak ] ∈ D/∼ exists and d̂( k [Ak ]) = k d̂([Ak ]). The gist of the proof: ‘lagged’ subsets. Jarno Talponen (UEF) On generalized measure algebras June, 2015 6 / 12 Structure of the proof 1/2: σ-additivity of d on the cosets Lemma With the above notations the mapping d̂ is countably additive in the following sense: Suppose that ([Ak ])k∈N ⊂ D/ -increasing W W∼ is a N W sequence. Then k [Ak ] ∈ D/∼ exists and d̂( k [Ak ]) = k d̂([Ak ]). The gist of the proof: ‘lagged’ subsets. Version of the main lemma in the paper in more general form: N L, [0, 1] G , {1, . . . , n}-averages ϕn , lim limF . Jarno Talponen (UEF) On generalized measure algebras June, 2015 6 / 12 Structure of the proof 2/2: Dynkin lemma argument We will apply the argument of the Dynkin-Sierpinski π-λ-lemma. We call a subset ∆ ⊂ D/∼ a d-system if it satisfies the following conditions: Jarno Talponen (UEF) On generalized measure algebras June, 2015 7 / 12 Structure of the proof 2/2: Dynkin lemma argument We will apply the argument of the Dynkin-Sierpinski π-λ-lemma. We call a subset ∆ ⊂ D/∼ a d-system if it satisfies the following conditions: (i) [N] ∈ ∆; Jarno Talponen (UEF) On generalized measure algebras June, 2015 7 / 12 Structure of the proof 2/2: Dynkin lemma argument We will apply the argument of the Dynkin-Sierpinski π-λ-lemma. We call a subset ∆ ⊂ D/∼ a d-system if it satisfies the following conditions: (i) [N] ∈ ∆; (ii) For each [A], [B] ∈ ∆, [A] N [B], we have [B \ A] ∈ ∆; Jarno Talponen (UEF) On generalized measure algebras June, 2015 7 / 12 Structure of the proof 2/2: Dynkin lemma argument We will apply the argument of the Dynkin-Sierpinski π-λ-lemma. We call a subset ∆ ⊂ D/∼ a d-system if it satisfies the following conditions: (i) [N] ∈ ∆; (ii) For each [A], [B] ∈ ∆, [A] N [B], we have [B \ A] ∈ ∆; (iii) For each [A], [B] ∈ ∆, A ∩ B = ∅, we have [A ∪ B] ∈ ∆; Jarno Talponen (UEF) On generalized measure algebras June, 2015 7 / 12 Structure of the proof 2/2: Dynkin lemma argument We will apply the argument of the Dynkin-Sierpinski π-λ-lemma. We call a subset ∆ ⊂ D/∼ a d-system if it satisfies the following conditions: (i) (ii) (iii) (iv) [N] ∈ ∆; For each [A], [B] ∈ ∆, [A] N [B], we have [B \ A] ∈ ∆; For each [A], [B] ∈ ∆, A ∩ B = ∅, we have [A ∪ B] ∈ ∆; If (Ak ) ⊂ ∆ is an increasing sequence in the order inherited from D/∼ , then the least upper bound A for this sequence exists in D/∼ and moreover A ∈ ∆. Jarno Talponen (UEF) On generalized measure algebras June, 2015 7 / 12 Structure of the proof 2/2: Dynkin lemma argument We will apply the argument of the Dynkin-Sierpinski π-λ-lemma. We call a subset ∆ ⊂ D/∼ a d-system if it satisfies the following conditions: (i) (ii) (iii) (iv) [N] ∈ ∆; For each [A], [B] ∈ ∆, [A] N [B], we have [B \ A] ∈ ∆; For each [A], [B] ∈ ∆, A ∩ B = ∅, we have [A ∪ B] ∈ ∆; If (Ak ) ⊂ ∆ is an increasing sequence in the order inherited from D/∼ , then the least upper bound A for this sequence exists in D/∼ and moreover A ∈ ∆. Let ∆ be the intersection of all d-systems in D/∼ containing F/∼ . Jarno Talponen (UEF) On generalized measure algebras June, 2015 7 / 12 Structure of the proof 2/2: Dynkin lemma argument We will apply the argument of the Dynkin-Sierpinski π-λ-lemma. We call a subset ∆ ⊂ D/∼ a d-system if it satisfies the following conditions: (i) (ii) (iii) (iv) [N] ∈ ∆; For each [A], [B] ∈ ∆, [A] N [B], we have [B \ A] ∈ ∆; For each [A], [B] ∈ ∆, A ∩ B = ∅, we have [A ∪ B] ∈ ∆; If (Ak ) ⊂ ∆ is an increasing sequence in the order inherited from D/∼ , then the least upper bound A for this sequence exists in D/∼ and moreover A ∈ ∆. Let ∆ be the intersection of all d-systems in D/∼ containing F/∼ . The modification of the π-λ-lemma argument gives that ∆ is essentially a σ-algebra. Jarno Talponen (UEF) On generalized measure algebras June, 2015 7 / 12 Spaces of the type Lp (L, ϕ) Speculative part of the paper. What is Lp (L, ϕ) where ϕ is a submeasure on a lattice L? Jarno Talponen (UEF) On generalized measure algebras June, 2015 8 / 12 Spaces of the type Lp (L, ϕ) Speculative part of the paper. What is Lp (L, ϕ) where ϕ is a submeasure on a lattice L? It should be the completion of a suitable normed space of ‘simple functions’. Except that the space is pointless - not a genuine function space. Jarno Talponen (UEF) On generalized measure algebras June, 2015 8 / 12 Spaces of the type Lp (L, ϕ) Speculative part of the paper. What is Lp (L, ϕ) where ϕ is a submeasure on a lattice L? It should be the completion of a suitable normed space of ‘simple functions’. Except that the space is pointless - not a genuine function space. That is mimicking a possible (re)construction of Lp (µ) from the measure algebra (A, µ), where A = Σ/Ker(µ). Jarno Talponen (UEF) On generalized measure algebras June, 2015 8 / 12 Spaces of the type Lp (L, ϕ) Speculative part of the paper. What is Lp (L, ϕ) where ϕ is a submeasure on a lattice L? It should be the completion of a suitable normed space of ‘simple functions’. Except that the space is pointless - not a genuine function space. That is mimicking a possible (re)construction of Lp (µ) from the measure algebra (A, µ), where A = Σ/Ker(µ). We start with the space c00 (L) and denote its canonical Hamel basis unit vectors by eA , A ∈ L. Jarno Talponen (UEF) On generalized measure algebras June, 2015 8 / 12 Spaces of the type Lp (L, ϕ) Speculative part of the paper. What is Lp (L, ϕ) where ϕ is a submeasure on a lattice L? It should be the completion of a suitable normed space of ‘simple functions’. Except that the space is pointless - not a genuine function space. That is mimicking a possible (re)construction of Lp (µ) from the measure algebra (A, µ), where A = Σ/Ker(µ). We start with the space c00 (L) and denote its canonical Hamel basis unit vectors by eA , A ∈ L. This vector space by itself is not ‘realistic’ model for ‘simple functions’ because there is a spike supported on 0 (empty set). Also, c00 (L) does not recognize the possible overlap of the supports. Jarno Talponen (UEF) On generalized measure algebras June, 2015 8 / 12 Tensorification To fix these issues we can use an approach similar to the tensor space constructions. Jarno Talponen (UEF) On generalized measure algebras June, 2015 9 / 12 Tensorification To fix these issues we can use an approach similar to the tensor space constructions. Let ∆ ⊂ c00 (L) be the linear subspace given by ∆ = [e0 ] + span((eA + eB ) − (eA∨B + eA∧B ) : A, B ∈ L}. Jarno Talponen (UEF) On generalized measure algebras June, 2015 9 / 12 Tensorification To fix these issues we can use an approach similar to the tensor space constructions. Let ∆ ⊂ c00 (L) be the linear subspace given by ∆ = [e0 ] + span((eA + eB ) − (eA∨B + eA∧B ) : A, B ∈ L}. We let q : c00 (L) → c00 (L)/∆ be the canonical quotient mapping. Jarno Talponen (UEF) On generalized measure algebras June, 2015 9 / 12 Tensorification To fix these issues we can use an approach similar to the tensor space constructions. Let ∆ ⊂ c00 (L) be the linear subspace given by ∆ = [e0 ] + span((eA + eB ) − (eA∨B + eA∧B ) : A, B ∈ L}. We let q : c00 (L) → c00 (L)/∆ be the canonical quotient mapping. Write X = c00 (L)/∆ and we denote by a ⊗ A := q(aeA ) ∈ X , a ∈ R, A ∈ L. Note that X is the space of vectors of the form X ai ⊗ Ai , ai ∈ R, Ai ∈ L, I finite. i∈I Jarno Talponen (UEF) On generalized measure algebras June, 2015 9 / 12 Auxiliary vector preorder Let v be the preorder on X generated by the following conditions: Jarno Talponen (UEF) On generalized measure algebras June, 2015 10 / 12 Auxiliary vector preorder Let v be the preorder on X generated by the following conditions: (i) v satisfies the axioms of a partial order of a vector lattice, except possibly anti-symmetry; Jarno Talponen (UEF) On generalized measure algebras June, 2015 10 / 12 Auxiliary vector preorder Let v be the preorder on X generated by the following conditions: (i) v satisfies the axioms of a partial order of a vector lattice, except possibly anti-symmetry; (ii) a ⊗ A v b ⊗ A whenever a ≤ b; Jarno Talponen (UEF) On generalized measure algebras June, 2015 10 / 12 Auxiliary vector preorder Let v be the preorder on X generated by the following conditions: (i) v satisfies the axioms of a partial order of a vector lattice, except possibly anti-symmetry; (ii) a ⊗ A v b ⊗ A whenever a ≤ b; (iii) 1 ⊗ A v 1 ⊗ B whenever A ≤ B in the intrinsic partial order of L. Jarno Talponen (UEF) On generalized measure algebras June, 2015 10 / 12 Auxiliary vector preorder Let v be the preorder on X generated by the following conditions: (i) v satisfies the axioms of a partial order of a vector lattice, except possibly anti-symmetry; (ii) a ⊗ A v b ⊗ A whenever a ≤ b; (iii) 1 ⊗ A v 1 ⊗ B whenever A ≤ B in the intrinsic partial order of L. We define a semi-norm on X by ! ρ X ai ⊗ Ai i = inf X Jarno Talponen (UEF) k !1 p |bk |p ϕ(Bk ) : ± X ai ⊗ Ai v i On generalized measure algebras X |bk | ⊗ Bk . k June, 2015 10 / 12 Auxiliary vector preorder Let v be the preorder on X generated by the following conditions: (i) v satisfies the axioms of a partial order of a vector lattice, except possibly anti-symmetry; (ii) a ⊗ A v b ⊗ A whenever a ≤ b; (iii) 1 ⊗ A v 1 ⊗ B whenever A ≤ B in the intrinsic partial order of L. We define a semi-norm on X by ! ρ X ai ⊗ Ai i = inf X k !1 p |bk |p ϕ(Bk ) : ± X ai ⊗ Ai v i X |bk | ⊗ Bk . k Indeed, it is easy to see that this is a semi-norm; the triangle inequality follows from the condition that x + y v v + w whenever x v v and y v w . Jarno Talponen (UEF) On generalized measure algebras June, 2015 10 / 12 Non-distributive Lp space We define Lp (L, ϕ) to be the completion of (X /ker(ρ), ρ(·)). Jarno Talponen (UEF) On generalized measure algebras June, 2015 11 / 12 Non-distributive Lp space We define Lp (L, ϕ) to be the completion of (X /ker(ρ), ρ(·)). Jarno Talponen (UEF) On generalized measure algebras June, 2015 11 / 12 Non-distributive Lp space We define Lp (L, ϕ) to be the completion of (X /ker(ρ), ρ(·)). Theorem Let 1 ≤ p < ∞, L be an orthomodular lattice with an order-preserving map ϕ : L → [0, 1], as above. Let (Ω, Σ, µ) be a probability space and Σ0 ⊂ Σ a Boolean algebra which σ-generates Σ. Let us assume that ϕ(M ∨ N) = ϕ(M) + ϕ(N) whenever N ≤ M ⊥ . Suppose that there is an order-embedding : Σ0 → L such that µ(M) = ϕ(M) for all M ∈ Σ0 . (We are not assuming here that respects the orthocomplementation operation.) Then X X ai [1Ai ]a.e. → 7 ai ⊗ (Ai ), Ai ∈ Σ0 = i i extends to a linear (into) isometry Lp (Ω, Σ, µ) → Lp (L, ϕ). Jarno Talponen (UEF) On generalized measure algebras June, 2015 11 / 12 Some related references A. Blass, R. Frankiewicz, G. Plebanek, C. Ryll-Nardzewski, A note on extensions of asymptotic density. Proc. Amer. Math. Soc. 129 (2001), 3313–3320. C.R. Buck, The measure theoretic approach to density. Amer. J. Math. 68, (1946), 560–580. E.F. Buck, C.R. Buck, A note on finitely-additive measures. Amer. J. Math. 69, (1947), 413–420. D.H. Fremlin, Measure Theory. Torres Fremlin 2000. P. de Lucia and P. Morales, A non-commutative version of a theorem of Marczewski for submeasures. Studia Math, 101 (1992), 123–138. M. Di Nasso, Fine asymptotic densities for sets of natural numbers. Proc. Amer. Math. Soc. 138 (2010), 2657–2665. Jarno Talponen (UEF) On generalized measure algebras June, 2015 12 / 12