Giry monad

The Giry monad, like every monad, consists of three structures: • A functorial assignment, which in this case assigns to a measurable space X a space of probability measures PX over it; • A natural map \delta_X:X\to PX called the unit, which in this case assigns to each element of a space the Dirac measure over it; • A natural map \mathcal{E}_X:PPX\to PX called the multiplication, which in this case assigns to each probability measure over probability measures its expected value. The space of probability measures Let (X, \mathcal{F}) be a measurable space. Denote by PX the set of probability measures over (X, \mathcal{F}). We equip the set PX with a sigma-algebra as follows. First of all, for every measurable set A\in \mathcal{F}, define the map \varepsilon_A:PX\to\mathbb{R} by p\longmapsto p(A). We then define the sigma algebra \mathcal{PF} on PX to be the smallest sigma-algebra which makes the maps \varepsilon_A measurable, for all A\in\mathcal{F} (where \mathbb{R} is assumed equipped with the Borel sigma-algebra). The assignment (X,\mathcal{F})\mapsto (PX,\mathcal {PF}) is part of an endofunctor on the category of measurable spaces, usually denoted again by P. Its action on morphisms, i.e. on measurable maps, is via the pushforward of measures. Namely, given a measurable map f:(X,\mathcal{F})\to(Y,\mathcal{G}), one assigns to f the map f_*:(PX,\mathcal {PF})\to(PY,\mathcal {PG}) defined by :f_*p\,(B)=p(f^{-1}(B)) for all p\in PX and all measurable sets B\in\mathcal{G}. The Dirac delta map Given a measurable space (X,\mathcal{F}), the map \delta:(X,\mathcal{F})\to(PX,\mathcal{PF}) maps an element x\in X to the Dirac measure \delta_x\in PX, defined on measurable subsets A\in\mathcal{F} by : \delta_x(A) = 1_A(x) = \begin{cases} 1 & \text{if }x\in A, \\ 0 & \text{if }x\notin A. \end{cases} The expectation map Let \mu\in PPX, i.e. a probability measure over the probability measures over (X,\mathcal{F}). We define the probability measure \mathcal{E}\mu\in PX by : \mathcal{E}\mu(A) = \int_{PX} p(A)\,\mu(dp) for all measurable A\in\mathcal{F}. This gives a measurable, natural map \mathcal{E}:(PPX,\mathcal{PPF})\to(PX,\mathcal{PF}). Example: mixture distributions A mixture distribution, or more generally a compound distribution, can be seen as an application of the map \mathcal{E}. Let's see this for the case of a finite mixture. Let p_1,\dots,p_n be probability measures on (X,\mathcal{F}), and consider the probability measure q given by the mixture : q(A) = \sum_{i=1}^n w_i\,p_i(A) for all measurable A\in\mathcal{F}, for some weights w_i\ge 0 satisfying w_1+\dots+w_n=1. We can view the mixture q as the average q=\mathcal{E}\mu, where the measure on measures \mu\in PPX, which in this case is discrete, is given by : \mu = \sum_{i=1}^n w_i\,\delta_{p_i} . More generally, the map \mathcal{E}:PPX\to PX can be seen as the most general, non-parametric way to form arbitrary mixture or compound distributions. The triple (P,\delta,\mathcal{E}) is called the Giry monad. ==Relationship with Markov kernels==

One of the properties of the sigma-algebra \mathcal{PF} is that given measurable spaces (X,\mathcal{F}) and (Y,\mathcal{G}), we have a bijective correspondence between measurable functions (X,\mathcal{F})\to(PY,\mathcal{PG}) and Markov kernels (X,\mathcal{F})\to(Y,\mathcal{G}). This allows to view a Markov kernel, equivalently, as a measurably parametrized probability measure. In more detail, given a measurable function f:(X,\mathcal{F})\to(PY,\mathcal{PG}), one can obtain the Markov kernel f^\flat:(X,\mathcal{F})\to(Y,\mathcal{G}) as follows, : f^\flat(B|x) = f(x)(B) for every x\in X and every measurable B\in\mathcal{G} (note that f(x)\in PY is a probability measure). Conversely, given a Markov kernel k:(X,\mathcal{F})\to(Y,\mathcal{G}), one can form the measurable function k^\sharp:(X,\mathcal{F})\to(PY,\mathcal{PG}) mapping x\in X to the probability measure k^\sharp(x)\in PY defined by : k^\sharp(x)(B) = k(B|x) for every measurable B\in\mathcal{G}. The two assignments are mutually inverse. From the point of view of category theory, we can interpret this correspondence as an adjunction : \mathrm{Hom}_\mathrm{Meas} (X,PY) \cong \mathrm{Hom}_\mathrm{Stoch} (X,Y) between the category of measurable spaces and the category of Markov kernels. In particular, the category of Markov kernels can be seen as the Kleisli category of the Giry monad. ==Product distributions==

Given measurable spaces (X,\mathcal{F}) and (Y,\mathcal{G}), one can form the measurable space (PX,\mathcal{PX})\times (PY,\mathcal{PY})=(X\times Y, \mathcal{F}\times\mathcal{G}) with the product sigma-algebra, which is the product in the category of measurable spaces. Given probability measures p\in PX and q\in PY, one can form the product measure p\otimes q on (X\times Y, \mathcal{F}\times\mathcal{G}). This gives a natural, measurable map : (PX,\mathcal{PF})\times (PY,\mathcal{PG})\to \big(P(X\times Y), \mathcal{P(F\times G)}\big) usually denoted by \nabla or by \otimes. The map \nabla:PX\times PY\to P(X\times Y) is in general not an isomorphism, since there are probability measures on X\times Y which are not product distributions, for example in case of correlation. However, the maps \nabla:PX\times PY\to P(X\times Y) and the isomorphism 1\cong P1 make the Giry monad a monoidal monad, and so in particular a commutative strong monad. ==Further properties==

• If a measurable space (X,\mathcal{F}) is standard Borel, so is (PX,\mathcal{PF}). Therefore, the Giry monad restricts to the full subcategory of standard Borel spaces. For example, for [0,\infty], the structure map e:P[0,\infty]\to [0,\infty] is given by : p \longmapsto \int_{[0,\infty)} x\,p(dx) :whenever p is supported on [0,\infty) and has finite expected value, and e(p)=\infty otherwise. == See also ==