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We know the functor sending a measurable space to its measurable space of probability measures is a monad. Is this true also if we replace 'probability measures' with arbitrary measures?
Put in other words, is there a point in the construction in which (or at least ) is actually crucial? I'm too lazy to work it out now so I'm asking here to see if someone has a ready answer for me
At first I thought finite measures were required. If T is your monad, you need a map TTX TX, which converts a measure on the space of measures on X into a measure on X. We get this by integration. If we allow infinite measures, this integral could be infinite. But now I think that's fine: there's a measure on X that sends every nonempty set to , for example, so a result like that is allowed.
There was some discussion of this issue at theory: probability / improper priors. @Sam Staton linked to his paper where he uses a category of "s-finite" kernels. (s-finite measures are a particularly well-behaved class of possibly-infinite measures.)
I guess that's more about defining a Markov category of s-finite kernels directly, rather than as the Kleisli category of a monad, though.
@Nathaniel Virgo does s-finite mean -finite?
No, it's different! https://en.wikipedia.org/wiki/S-finite_measure
I'm not really an expert on this measure-theoretic stuff though - I'm hoping someone else will chime in
Uh that's a cool concept, I've never seen it before!
John Baez said:
At first I thought finite measures were required. If T is your monad, you need a map TTX TX, which converts a measure on the space of measures on X into a measure on X. We get this by integration. If we allow infinite measures, this integral could be infinite. But now I think that's fine: there's a measure on X that sends every nonempty set to , for example, so a result like that is allowed.
Btw this is also where I thought problem could arise, though as you point out... not really! Though I can't still swear that there are no problem convolving one measure over the other when they could be infinite.
In Lean's mathlib library this monad is formalized without the restriction to probability (or bounded) measures.
https://github.com/leanprover-community/mathlib/blob/master/src/measure_theory/giry_monad.lean
Thanks Reid! I guess this settles the question
Nice! A good general principle: is not a problem when dealing with sums or integrals unless you also have negative numbers around.
Dealing with signed possibly-infinite measures is much more tricky than dealing with possibly-infinite measures, because there's no good definition of .
Indeed
But there's never an ambiguity when adding (possibly infinite, even uncountable) sets of numbers in .
We can talk about "infinitary Lawvere theories" where we allow operations of arbitrary arity (though it's typical to bound the arity by some cardinal or other... take an inaccessible cardinal if you want).
So, we can talk about an "infinitary commutative monoid", in which sums of arbitrary cardinality are well-defined, and infinitary versions of the associative and commutative laws hold.
Then is an infinitary commutative monoid, and so is .
Measure theory uses the latter.
Wow this is cool!
Thanks! Here's an important and fun fact: if you add infinitely many numbers in and get a finite answer, at most countably many of these numbers can be nonzero.
then what do you call integration? :thinking:
jk
John's fact is why we need measure theory in the first place. It means that if you try to assign probabilities to elements of a set directly, only countably many can ever be nonzero
@sarahzrf Infinitessimals are non-nonzero, I think.
nice :)
read my mind