nLab superconvex space

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Contents

Idea

The notion of “superconvex spaces” generalizes the idea of convex spaces by replacing finite affine sums with countable affine sums.

The category of superconvex spaces is the category of algebras for the countable distribution monad DD defined on Set\mathbf{Set} by:

For XX a set let DXD X be the set whose elements are functions p:X[0,1]p:X\to[0,1] such that

  • p(x)0p(x)\ne 0 for only countably many xx, and

  • xXp(x)=1\sum_{x\in X} p(x)=1. (The limit of the countable sum is one.)

Note that the sum above is countable if one excludes all the zero addenda.

The elements of DXD X are called countable distributions or countably-supported probability measures over XX.

Given a function f:XYf:X\to Y, one defines the pushforward Df:DXDYD f:D X\to D Y as follows. Given pDXp\in D X, then (Df)(p)DY(D f)(p)\in D Y is the function

y xf 1(y)p(x). y \;\mapsto\; \sum_{x\in f^{-1}(y)} p(x) .

(Note that, up to zero addenda, the sum above is again countable. Moreover, once we have defined countably affine, note that the pushforward map is countably affine.)

Definition

Let 𝒢()\mathcal{G}(\mathbb{N}) denote the set of all probability measures on the set of natural numbers, hence every p\mathbf{p} can be represented as p= ip iδ i\mathbf{p} = \sum_{i \in \mathbb{N}} p_i \delta_i where ip i=1\sum_{i \in \mathbb{N}} p_i=1 with each p i[0,1]p_i \in [0,1]. Here 𝒢\mathcal{G} is the Giry monad, but because we want to forget the σ\sigma-algebra associated with the measurable space 𝒢(𝕄)\mathcal{G}(\mathbb{M}) we often write Δ \Delta_{\mathbb{N}} for its underlying set. That set may be regarded as the countably infinite-dimensional simplex, as such it is the prototypical example of a superconvex space.

Given any set AA, a sequence a:A\mathbf{a} \colon \mathbb{N} \rightarrow A, and any p𝒢()\mathbf{p} \in \mathcal{G}(\mathbb{N}), we refer to the formal sum ip ia i\sum_{i \in \mathbb{N}} p_i a_i as a countably affine sum of elements of AA, and for brevity we use the notation ip ia i\sum_{i\in \mathbb{N}} p_i a_i to refer to a countably affine sum dropping the explicit reference to the condition that the limit of partial sums i=0 Np i\sum_{i=0}^N p_i converges to one. An alternative notation to the countable affine sum notation is to use the integral notation

adp ip ia i. \int_{\mathbb{N}} \mathbf{a} \, d\mathbf{p} \;\coloneqq\; \sum_{i \in \mathbb{N}} p_i a_i.

Definition

(superconvex spaces)
We say a set AA has the structure of a superconvex space if it comes equipped with a function

st A : 𝒢()×Set(,A) A (p,a) adp \begin{array}{ccccc} st_A &\colon& \mathcal{G}{(\mathbb{N})} \times \Set(\mathbb{N}, A) & \rightarrow& A \\ && (\mathbf{p}, \mathbf{a}) & \mapsto & \int_{\mathbb{N}} \mathbf{a} \, d\mathbf{p} \end{array}

such that the following axiom is satisfied:

  • Axiom. If p𝒢()\mathbf{p} \in \mathcal{G}(\mathbb{N}) and Q:𝒢()\mathbf{Q}: \mathbb{N} \rightarrow \mathcal{G}(\mathbb{N}) is a sequence of probability measures on (,𝒫())(\mathbb{N}, \mathcal{P}(\mathbb{N})) then

    j( adQ j)dp= ad( jQ dp). \textstyle{\int_{j \in \mathbb{N}}} \big( \int_{\mathbb{N}} \mathbf{a} \, d\mathbf{Q}^j \big) \, d\mathbf{p} \;=\; \textstyle{\int_{\mathbb{N}}} \mathbf{a} \, d\big( \textstyle{\int_{j \in \mathbb{N}}} \mathbf{Q}^{\bullet} \, d\mathbf{p} \big) \,.

Remark

The axiom uses the pushforward measure 𝒢(Q)p𝒢 2\mathcal{G}(\mathbf{Q})\mathbf{p} \in \mathcal{G}^2{\mathbb{N}} and the natural transformation μ\mu of the Giry monad at component \mathbb{N}, μ :𝒢 2()𝒢()\mu_{\mathbb{N}}: \mathcal{G}^2(\mathbb{N}) \rightarrow \mathcal{G}(\mathbb{N}), which yields the probability measure on the measurable space (,𝒫)(\mathbb{N}, \mathcal{P}{\mathbb{N}}) whose value at the measurable set {j}\{j\} is given by the composite of measurable maps

Definition

(category of superconvex spaces)
A morphism of superconvex spaces, called a countably affine map, is a set function m:ABm: A \rightarrow B such that

m( adp)= (ma)dp, m \big( \textstyle{\int_{\mathbb{N}}} \mathbf{a} \, d\mathbf{p} \big) \;=\; \textstyle{\int_{\mathbb{N}}} (m \circ \mathbf{a}) \, d\mathbf{p} \,,

where the composite mam \circ \mathbf{a} gives the sequence in BB with component m(a i)m(a_i). Composition of countably affine maps is the set-theoretical composition.

Superconvex spaces with morphisms the countably affine maps thus form a category denoted SCvx\mathbf{SCvx}.

Probability Amplitudes

In physics, superconvex spaces have been referred to as strong convex spaces, and since probability amplitudes are employed there one makes use of the 2\ell_2-norm instead of the tradition ‘’ 1\ell_1-norm’‘ which is used above. By using

𝒢()={p:D 2|lim N( i=1 Np ip i )=1}, \mathcal{G}(\mathbb{N}) \;=\; \Big\{ \mathbf{p} \colon \mathbb{N} \rightarrow \mathbf{D}_2 \Big\vert \lim_{N \rightarrow \infty} \big( \textstyle{\sum_{i=1}^N} p_i p_i^{\star} \big) \,=\, 1 \Big\} \,,

where

D 2{re ıθ|r[0,1],andθ[0,2π)} \mathbf{D}_2 \;\coloneqq\; \big\{ r e^{\imath \theta} \in \mathbb{C} \,\big\vert\, r \in [0,1], \text{and} \theta \in [0,2 \pi) \big\}

and p i p_i^{\star} is the complex conjugate of p ip_i, applied to the above axioms one obtains superconvex spaces useful for physics.

Properties

Lemma

For every sequence a:A\mathbf{a} \colon \mathbb{N} \rightarrow A and every jj \in \mathbb{N} the property

adδ j=a j \textstyle{\int_{\mathbb{N}}} \mathbf{a} \, \, d\delta_j \;=\; a_j

holds.

Proof

Choose the constant sequence Q:𝒢\mathbf{Q}: \mathbb{N} \rightarrow \mathcal{G}\mathbb{N} with value δ j\delta_j applied to the axiom yields the result.

This lemma is often taken as a separate axiom.

The most basic property of superconvex spaces, is

Lemma

For AA any superconvex space every countably affine map mSCvx(Δ ,A)m \in \SCvx(\Delta_{\mathbb{N}}, A) is uniquely specified by a sequence in AA, hence we have SCvx(Δ ,A)Set(,A)\SCvx(\Delta_{\mathbb{N}}, A) \cong \Set(\mathbb{N},A).

Proof

Every element pΔ \mathbf{p} \in \Delta_{\mathbb{N}} has a unique representation as a countable affine sum p= ip iδ i\mathbf{p} = \sum_{i \in \mathbb{N}} p_i \delta_i, and hence a countably affine map m:Δ Am:\Delta_{\mathbb{N}} \rightarrow A is uniquely determined by where it maps each Dirac measure δ i\delta_i. Thus im(δ i)i \mapsto m(\delta_i) specifies a sequence in AA.

We denote the bijective correspondence SCvx(Δ ,A)Set(,A)\SCvx(\Delta_{\mathbb{N}}, A) \cong \Set(\mathbb{N},A) by aa\langle \mathbf{a} \rangle \leftrightarrow \mathbf{a}, where a:A\mathbf{a}: \mathbb{N} \rightarrow A specifies a sequence in AA.

Lemma

A function f:f \colon \mathbb{N} \rightarrow \mathbb{N} is a countably affine map if and only if ff is monotone, i<ji \lt j implies f(i)f(j)f(i) \le f(j).

Proof

Necessary condition. Suppose that f:f: \mathbb{N} \rightarrow \mathbb{N} is a countably affine map. Let i<ji \lt j. By the superconvex space structure on \mathbb{N} it follows, for all α(0,1)\alpha \in (0,1), that αi+(1α)j=i\alpha i + (1-\alpha) j = i . If ff is not monotone then there exist a pair of elements i,ji,j \in \mathbb{N} such that i<ji \lt j with f(j)<f(i)f(j) \lt f(i). This implies, for all α(0,1)\alpha \in (0,1), that

f(j)=αf(i)+(1α)f(j)<f(αi+(1α)j)=f(i), f(j)= \alpha f(i) + (1-\alpha) f(j) \lt f(\alpha i + (1-\alpha) j ) =f(i),

which contradicts our hypothesis that ff is a countably affine map.

Sufficient condition. Suppose ff is a monotone function, and that we are given an arbitrary countably affine sum ip ii=n\sum_{i \in \mathbb{N}} p_i i = n in \mathbb{N}, so that for all i=0,1,,n1i=0,1,\ldots,n-1 we have p i=0p_i=0. Since the condition defining the superconvex structure is conditioned on the property p i0p_i \ne 0, the countably affine sum is not changed by removing any number of terms ii in the countable sum whose coefficient p i=0p_i=0. Hence for all jj such that n<jn\lt j it follows that f(n)f(j)f(n) \le f(j) so that

f( i=0 p ii)=f(n)= i=n p if(i), f\big( \textstyle{\sum_{i=0}^{\infty}} p_i \, i \big) \,=\, f(n) \,=\, \textstyle{\sum_{i=n}^{\infty}} p_i f(i) \,,

where the last equality follows from the definition of the superconvex space structure on \mathbb{N}.

Lemma

The standard free space construction can be applied to superconvex spaces to obtain an adjoint pair :SetSCvx:𝒰\mathcal{F}:\mathbf{Set} \leftrightarrows \mathbf{SCvx}: \mathcal{U} where (A)\mathcal{F}(A) consists of all formal countable affine sums, adp:= ip ia i\int_{\mathbb{N}} \mathbf{a} \, d\mathbf{p} := \sum_{i \in \mathbb{N}}p_i a_i for p𝒢\mathbf{p} \in \mathcal{G}{\mathbb{N}} and aSet(,A)\mathbf{a} \in \mathbf{Set}(\mathbb{N},A), modulo the relations

j( iadQ i)dp jad( iQ dp)QSet(,𝒢), \textstyle{\int_{j \in \mathbb{N}}} \big( \textstyle{\int_{i \in \mathbb{N}}} \mathbf{a} \, d\mathbf{Q}^i \big) \, d\mathbf{p} \;\cong\; \textstyle{\int_{j \in \mathbb{N}}} \mathbf{a} \, d \big( \textstyle{\int_{i \in \mathbb{N}}} \mathbf{Q}^{\bullet} \, d\mathbf{p} \big) \quad\quad\quad \forall \, \mathbf{Q} \in \mathbf{Set}( \mathbb{N}, \mathcal{G}{\mathbb{N}}) \,,

so that the sole necessary axiom of a superconvex space is satisfied.

The monad arising from this adjunction, with the usual unit and counit maps (for the free and forgetful functors), is the countable distribution monad defined in the Idea section, and the category of algebras of that monad is superconvex spaces.

Proof

Note that the finite distribution monad also arises from the free functor and forgetful functor adjunction. (The verification that the finite and countable distributions arise from the free functor and forgetful functor is straight forward.)

A direct method to prove that the category of algebras of DD, Alg(D)Alg(D), is equivalent to the category of superconvex spaces is to show that the comparison functor Φ:SCvxAlg(D)\Phi: \mathbf{SCvx} \rightarrow Alg(D) has a two-sided inverse Ψ:Alg(D)SCvx\Psi: Alg(D) \rightarrow \mathbf{SCvx}. This functor is defined on objects by taking Ψ(α:DXX)\Psi( \alpha:D X \rightarrow X ) as the set XX with the superconvex structure defined by ip ix i=α( ip ix i)\sum_{i \in \mathbb{N}} p_i x_i = \alpha(\sum_{i \in \mathbb{N}} p_i x_i) where the countable sum on the right hand side is a formal countable sum, which is an element of DXD X. Given any map of algebras f:(X,h)(Y,k)f: (X,h) \rightarrow (Y,k) it follows, as shown by the (only) proof given on the Giry monad page is that the function ff, which we now view in Set\mathbf{Set}, is necessarily a countably affine map. (Simply replace the terms ip iδ x i\sum_{i \in \mathbb{N}}p_i \delta_{x_i} with the term ip ix i\sum_{i \in \mathbb{N}}p_i x_i which is an element in DXD X.)

The category SCvx\mathbf{SCvx} has all limits and colimits. Furthermore it is a symmetric monoidal closed category under the tensor product. The proof of the latter condition follows the proof by Meng, replacing finite sums with countable sums.

The full subcategory consisting of the single object Δ \Delta_{\mathbb{N}} is dense in SCvx\mathbf{SCvx}, and hence we can employ the restricted Yoneda embedding to view superconvex spaces as the functors A^=SCvx(,A)Set Δ op\widehat{A}=\mathbf{SCvx}(\cdot,A) \in \mathbf{Set}^{\Delta_{\mathbb{N}}^{op}}, where Δ \Delta_{\mathbb{N}} is viewed as a monoid.

An ideal in a superconvex space AA is a subset \mathcal{I} such that whenever a 0a_0 \in \mathcal{I} and ip ia i\sum_{i \in \mathbb{N}}p_i a_i is a countable affine sum with the coefficient of a 0a_0 nonzero then ip ia i\sum_{i \in \mathbb{N}}p_i a_i \in \mathcal{I}. Ideals are useful for defining functors to or from SCvx\mathbf{SCvx}.

Examples

Example

A fundamental superconvex space is the set \mathbb{N} with the superconvex space structure defined, for every sequence s:\mathbf{s}: \mathbb{N} \rightarrow \mathbb{N} by

sdp=inf i{s i|p i>0}. \textstyle{\int_{\mathbb{N}}} \mathbf{s} d\mathbf{p} \;=\; \inf_i \{\mathbf{s}_i \, | \, p_i \gt 0 \} \,.

That structure on \mathbb{N} shows that the function ϵ:𝒢()\epsilon: \mathcal{G}(\mathbb{N}) \rightarrow \mathbb{N} defined by ip iδ iinf i{i|p i>0}\sum_{i \in \mathbb{N}} p_i \delta_i \mapsto \inf_i \{i | p_i\gt 0\} is a countably affine map.

Example

As an example of the utility of ideals in a superconvex space we note that for 𝒢\mathcal{G} the Giry monad the measurable space 𝒢(X)\mathcal{G}(X), with the smallest σ\sigma-algebra such that the evaluation maps ev U:𝒢(X)[0,1]ev_U: \mathcal{G}(X) \rightarrow [0,1] are measurable for every measurable set UU in XX, has a superconvex space structure defined on it pointwise.

Note that if XX is any measurable space the maximal proper ideals of 𝒢X\mathcal{G}{X} are of the form ev U 1((0,1])ev_{U}^{-1}( (0,1]) or ev U 1([0,1))ev_U^{-1}([0,1)) for UXU\ne X a nonempty measurable set in XX.

To prove this, note that both (0,1](0,1] and [0,1)[0,1) are ideals in the superconvex space [0,1][0,1], with the natural superconvex space structure, and it follows that ev U 1([0,1))ev_{U}^{-1}( [0,1)) and ev U 1((0,1])ev_U^{-1}((0,1]) are ideals in 𝒢X\mathcal{G}{X}. (The preimage of an ideal under a countably affine map is an ideal in the domain space. The proof is the standard argument for ideals in any category.) Consider the ideal ev U 1([0,1))ev_U^{-1}( [0,1)). To show that this is a maximal proper ideal suppose that \mathcal{I} is another ideal of 𝒢X\mathcal{G}{X} such that ev U 1([0,1))⫋︀ev_U^{-1}( [0,1)) \varsubsetneqq \mathcal{I}. Every element PP \in \mathcal{I} which is not in ev U 1([0,1))ev_U^{-1}([0,1)) has the defining property that P(U c)=1P(U^c)=1. Now let Q𝒢XQ \in \mathcal{G}{X}. If Q𝒥Q \notin \mathcal{J} and Qev U 1([0,1))Q \notin ev_U^{-1}([0,1)) then Q(U c)1Q(U^c) \ne 1 which implies Qev U 1([0,1))⫋︀JQ \in ev_U^{-1}( [0,1)) \varsubsetneqq J which is self-contradictory. Thus 𝒥\mathcal{J} must be all of 𝒢X\mathcal{G}{X} which shows ev U 1([0,1))ev_U^{-1}([0,1)) is a maximal (proper) ideal. The argument that the ideal ev U 1((0,1])ev_U^{-1}( (0,1]) is a maximal ideal is similiar except we replace the condition P(U c)=1P(U^c)=1 in the above proof with P(U)=0P(U)=0.

If we restrict to the category of standard measurable spaces then every object has a countable generating basis and it is then clear that every ideal in 𝒢(X)\mathcal{G}(X) is a countable intersection of maximal ideals, and hence measurable. This implies, for example, that every countably affine map k:𝒢(X)k: \mathcal{G}(X) \rightarrow \mathbb{N} is also a measurable function with \mathbb{N} having the powerset σ\sigma-algebra. (The only ideals of \mathbb{N} are the principal ideals 01\downarrow \! 0 \subset \downarrow \! 1 \subset \ldots.)

Example

The one point compactification of the real line \mathbb{R}_{\infty}, with one point adjoined, denoted \infty, which satisfies the property that any countably affine sum ip ir i=\sum_{i \in \mathbb{N}} p_i r_i = \infty if either (1) r j=r_j = \infty and p j>0p_j \gt 0 for any index jj, or (2) the sequence of partial sums does not converge, is a superconvex space. The real line \mathbb{R} is not a super convexspace since we could take p i=12 ip_i = \frac{1}{2^i} and r i=2 i+1r_i = 2^{i+1} and the limit of the sequence does not exist in \mathbb{R}. Thus while \mathbb{R} is a convex space it is not a superconvex space.

The only nonconstant countably affine map j: 𝟚j: \mathbb{R}_{\infty} \rightarrow \mathbb{2} is given by j(u)=1j(u)=1 for all uu \in \mathbb{R} and j()=0j(\infty)=0 (for the superconvex space structure on 2\mathbf{2} determined by 120̲+121̲=0̲\frac{1}{2} \underline{0} + \frac{1}{2} \underline{1} = \underline{0}).

Example

A pathological space, useful for counterexamples, is given by the closed unit interval with the superconvex space structure defined by the infimum function, ip iu i:=inf i{u i|p i>0}\sum_{i \in \mathbb{N}} p_i u_i := inf_i \{ u_i | p_i \gt 0\}.

Example

Consider the probability monad on compact Hausdorff spaces, where the algebras are precisely the compact convex sets KK in locally convex topological vector spaces together with the barycenter maps β K:𝒫KK\beta_K:\mathcal{P}K\rightarrow K.

Given such a space KK we can endow it with a superconvex space structure by defining, for all p𝒢\mathbf{p} \in \mathcal{G}\mathbb{N}, countable affine sums by ip ik i:=β K( ip iδ k i)\sum_{i \in \mathbb{N}} p_i k_i := \beta_K( \sum_{i \in \mathbb{N}} p_i \delta_{k_i}) which, along with the pointwise superconvex space structure on 𝒫K\mathcal{P}K makes the barycenter map β K\beta_K a countably affine map.

To prove that this endows KK with a superconvex space structure note that β K(δ k i)=k i\beta_K(\delta_{k_i})= k_i for all k iKk_i \in K to obtain

ip iβ K(δ k i)= ip ik iβ K( ip iδ k i). \textstyle{\sum_{i \in \mathbb{N}}} p_i \beta_K(\delta_{k_i}) \;=\; \textstyle{\sum_{i \in \mathbb{N}}} p_i k_i \,\coloneqq\, \beta_K\big( \textstyle{\sum_{i \in \mathbb{N}}} p_i \delta_{k_i} \big) \,.

To prove that β K\beta_K is countably affine on 𝒫K\mathcal{P}K use the property that β Kμ K=β K𝒫β K\beta_K \circ \mu_K = \beta_K \circ \mathcal{P}\beta_K.

The method employed in this example is not restricted to locally convex compact Hausdorff spaces. It shows that the algebras of a probability monad are a superconvex space. That implication is the motivation for the next example.

References

The notion of superconvex spaces originates with:

The proof that SCvx\mathbf{SCvx} has no cogenerator is due to:

The fact that SCvx\mathbf{SCvx} is a symmetric monoidal argument can be proven the same way it is for convex spaces simply by replacing the finite affine sums with countable affine sums. That proof was given by

  • Xiao-qing Meng, Categories of convex sets and of metric spaces with applications to stochastic programming and related areas, PhD thesis (djvu)

Proposition 1.2 in

is particularly useful for viewing superconvex spaces as positively convex spaces which are somewhat easier to work with because the condition ip i=1\sum_{i \in \mathbb{N}}p_i=1 is replaced by the inequality 1\le 1.

The fact that the functor Σ:ΩStd 2\mathbf{\Sigma}: \mathbf{\Omega} \rightarrow \mathbf{Std}_2 is a codense functor can be found in

although several aspects, such as the construction with the right-Kan is incorrect.

For purposes of constructing models of complex systems using superconvex spaces the construction given in Example 6.1 of the following article applies equally well to superconvex spaces.

The term strong convex space was employed in:

  • George Mackey, p. 68 of: The Mathematical Foundations of Quantum Mechanics: a Lecture-note Volume, Mathematical physics monograph series, Benjamin (1963), Dover (2004) [google books]

Last revised on July 5, 2024 at 07:50:49. See the history of this page for a list of all contributions to it.