# Natural Latents: The Math

Natural latents are a relatively elegant piece of math which we figured out over the past year, in our efforts to boil down and generalize various results and examples involving natural abstraction. In particular, this new framework handles approximation well, which was a major piece missing previously. This post will present the math of natural latents, with a handful of examples but otherwise minimal commentary. If you want the conceptual story, and a conceptual explanation for how this might connect to various problems, that will probably be in a future post.

While this post is not generally written to be a “concepts” post, it is generally written in the hope that people who want to use this math will see how to do so.

# 2-Variable Theorems

This section will present a simplified but less general version of all the main theorems of this post, in order to emphasize the key ideas and steps.

## Simplified Fundamental Theorem

Suppose we have:

A distribution over random variables

A latent variable which induces independence between and (first diagram below)

Another latent variable about which and give the same information (second diagram below)

Further, assume that mediates between and (third diagram below). This last assumption can typically be satisfied by construction in the minimality/maximality theorems below.

Then, claim: mediates between and .

### Intuition

Picture as a pipe between and . The only way any information can get from to is via that pipe (that’s the first diagram). is a piece of information which is present in both and - something we can learn from either of them (that’s the second pair of diagrams). Intuitively, the only way that can happen is if the information went through the pipe—meaning that we can also learn it from .

The third diagram rules out three-variable interactions which could mess up that intuitive picture—for instance, the case where one bit of is an xor of some independent random bit of and a bit of .

### Qualitative Example

Let and be the low-level states of two spatially-separated macroscopic chunks of an ideal gas at equilibrium. By looking at either of the two chunks, I can tell whether the temperature is above 50°C; call that More generally, the two chunks are independent given the pressure and temperature of the gas; call that .

Notice that is a function of , i.e. I can compute whether the temperature is above 50°C from the pressure and temperature itself, so mediates between and .

Some extensions of this example:

We could add more information to . For instance, could be the pressure and temperature and also the outcome of a die roll unrelated to the gas. Or, could be the entire low-level state of one of the two chunks.

We could remove information from For instance, could be a bit indicating whether the temperature is above 100°C

Intuitive mental picture: in general, can’t have “too little” information; it needs to include all information shared (even partially) across and . on the other hand, can’t have “too much” information; it can only include information which is fully shared across and .

### Proof

This is a diagrammatic proof; see Some Rules For An Algebra Of Bayes Nets for how to read it. (That post also walks through a version of this same proof as an example, so you should also look there if you want a more detailed walkthrough.)

(Throughout this post, denotes all components of except for .)

### Approximation

If the starting diagrams are satisfied approximately (i.e. they have small KL-divergence from the underlying distribution), then the final diagram is also approximately satisfied (i.e. has small KL-divergence from the underlying distribution). We can find quantitative bounds by propagating error through the proof:

Again, see the Algebra of Bayes Nets post for an unpacking of this notation and the proofs for each individual step.

### Qualitative Example

Note that our previous example realistically involved approximation: two chunks of an ideal gas won’t be *exactly* independent given pressure and temperature. But they’ll be independent to a very (very) tight approximation, so our conclusion will also hold to a very tight approximation.

### Quantitative Example

Suppose I have a biased coin, with bias . Alice flips the coin 1000 times, then takes the median of her flips. Bob also flips the coin 1000 times, then takes the median of his flips. We’ll need a prior on , so for simplicity let’s say it’s uniform on [0, 1].

Intuitively, so long as bias is unlikely to be very close to ½, Alice and Bob will find the same median with very high probability. So:

Let be Alice’ 1000 flips, and be Bob’s 1000 flips.

Let be the bias . Note that the flips are independent given , satisfying our first condition exactly.

Let be the median computed by either Bob or Alice (we’re assuming they are the same with high probability). Since the same median can be computed with high probability from either or , our second condition is approximately satisfied.

Since the median is computed as a deterministic function of , our third condition is satisfied exactly.

The fundamental theorem will then say that the bias approximately mediates between the median (either Alice’ or Bob’s) and the coinflips .

To quantify the approximation on the fundamental theorem, we first need to quantify the approximation on the second condition (the other two conditions hold exactly in this example, so their ‘s are 0). Let’s take to be Alice’ median. Alice’ flips mediate between Bob’s flips and the median exactly (i.e. ), but Bob’s flips mediate between Alice’ flips and the median (i.e. ) only approximately. Let’s compute that :

This is a dirichlet-multinomial distribution, so it will be cleaner if we rewrite in terms of , , and . is a function of , so the is

Assuming I simplified the gamma functions correctly, we then get:

(i.e. uniform over 0, …, n)

… and there’s only values of , so we can combine those expressions with a python script to evaluate everything:

```
import numpy as np
from scipy.special import gammaln, logsumexp, xlogy
n = 1000
p_N2 = np.ones(n+1)/(n+1)
N1 = np.outer(np.arange(n + 1), np.ones(n + 1))
N2 = np.outer(np.ones(n + 1), np.arange(n + 1))
# logP[N1|N2]; we're tracking log probs for numerical stability
lp_N1_N2 = (gammaln(n + 2) - gammaln(N2 + 1) - gammaln(n - N2 + 1) +
gammaln(n + 1) - gammaln(N1 + 1) - gammaln(n - N1 + 1) +
gammaln(N1 + N2 + 1) + gammaln(2*n - N1 - N2 + 1) - gammaln(2*n + 2))
# logP[\Lambda' = 0|N2] and logP[\Lambda' = 1|N2]
lp_lam0_N2 = logsumexp(lp_N1_N2[:500], axis=0)
lp_lam1_N2 = logsumexp(lp_N1_N2[500:], axis=0)
p_lam0_N2 = np.exp(lp_lam0_N2)
p_lam1_N2 = np.exp(lp_lam1_N2)
print(p_lam0_N2 + p_lam1_N2) # Check: these should all be 1.0
# ... aaaand then it's just the ol' -p * logp to get the expected entropy E[H(\Lambda')|N2]
H = - np.sum(p_lam0_N2 * lp_lam0_N2 * p_N2) - np.sum(p_lam1_N2 * lp_lam1_N2 * p_N2)
print(H / np.log(2)) # Convert to bits
```

The script spits out H = 0.058 bits. Sanity check: the main contribution to the entropy should be when is near 0.5, in which case the median should have roughly 1 bit of entropy. How close to 0.5? Well, with data points, posterior uncertainty should be of order , so the estimate of should be precise to roughly in either direction. is initially uniform on [0, 1], so distance 0.03 in either direction around 0.5 covers about 0.06 in prior probability, and the entropy should be roughly that times 1 bit, so roughly 0.06 bits. Which is exactly what we found (closer than this sanity check had any business being, really); sanity check passes.

Returning to the fundamental theorem: is 0, is 0, is roughly 0.058 bits. So, the theorem says that the coin’s true bias approximately mediates between the coinflips and Alice’ median, to within 0.12 bits.

Exercise: if we track the ’s a little more carefully through the proof, we’ll find that we can actually do somewhat better in this case. Show that, for this example, the coin’s true bias approximately mediates between the coinflips and Alice’ median to within , i.e. roughly 0.058 bits.

### Extension: More Stuff In The World

Let’s add another random variable to the setup, representing other stuff in the world. can have any relationship at all with , but must still induce independence between and . Further, must not give any more information about than was already available from or . Diagrams:

Then, as before, we conclude

For instance, in our ideal gas example, we could take to be the rest of the ideal gas (besides the two chunks and ). Then, our earlier conclusions still hold, even though there’s “more stuff” physically in between and and interacting with both of them.

The proof goes through much like before, with an extra Z dangling everywhere:

And, as before, we can propagate error through the proof to obtain an approximate version:

## Natural Latents

Suppose that a single latent variable (approximately) satisfies *both* the first two conditions of the Fundamental Theorem, i.e.

We call these the “naturality conditions”. If (approximately) satisfies both conditions, then we call a “natural latent”.

Example: if and are two spatially-separated mesoscopic chunks of an ideal gas, then the tuple (pressure, temperature) is a natural latent between the two. The first property (“mediation”) applies because pressure and temperature together determine all the intensive quantities of the gas (like e.g. density), and the low-level state of the gas is (approximately) independent across spatially-separated chunks given those quantities. The second property (“insensitivity”) applies because the pressure and temperature can be precisely and accurately estimated from either chunk.

### The Resample

Recall earlier that we said the condition

would be satisfied by construction in our typical use-case. It’s time for that construction.

The trick: if we have a natural latent , then construct a new natural latent by resampling conditional on (i.e. sample from ), independently of whatever other stuff we’re interested in. The resampled will have the same joint distribution with as does, so it will also be a natural latent, but it won’t have any “side-channel” interactions with other variables in the system—all of its interactions with everything else are mediated by , by construction.

From here on out, we’ll usually assume that natural latents have been resampled (and we’ll try to indicate that with the phrase “resampled natural latent”).

### Minimality & Maximality

Finally, we’re ready for our main theorems of interest about natural latents.

Assume that is a resampled natural latent over . Take *any* other latent about which and give (approximately) the same information, i.e.

Then, by the fundamental theorem:

So is, in this sense, the “most informative” latent about which and give the same information:

and give (approximately) the same information about , and for any other latent such that and give (approximately) the same information about tells us (approximately) everything which does about (and possibly more). This is the “maximality condition”.

Flipping things around: take any other latent which (approximately) induces independence between and :

By the fundamental theorem:

So is, in this sense, the “least informative” latent which induces independence between and :

(approximately) induces independence between and , and for any other latent which (approximately) induces independence between and , tells us (approximately) everything which does about (and possibly more). This is the “minimality condition”.

Further notes:

The minimality condition implies the natural latent conditions. Proof: take to be either or .

Both minimality and maximality imply a unique standard form (see appendix), so any resampled natural latent in standard form is also the unique natural and minimal and maximal latent in standard form. (In the approximate case, this becomes approximate uniqueness.) Furthermore, any natural latent can be transformed into standard form (as the phrase “standard form” implies).

In standard form, a natural latent is always approximately a deterministic function of . Specifically: .

Natural and minimal latents do not always exist, and maximal latents sometimes exist in cases where natural/minimal latents don’t. (For example, if and are two flips of a biased coin of unknown bias, then no natural latent exists to a good approximation. Intuitively, it’s because we don’t have enough data to precisely identify the bias which mediates between the datapoints.)

Basically everything about approximation and other parts of the world carries over to naturality/minimality/maximality.

### Example

In the ideal gas example, two chunks of gas are independent given (pressure, temperature), and (pressure, temperature) can be precisely estimated from either chunk. So, (pressure, temperature) is (approximately) a natural latent across the two chunks of gas. The resampled natural latent would be the (pressure, temperature) estimated by looking only at the two chunks of gas.

If there is some other latent which induces independence between the two chunks (like, say, the low-level state trajectory of all the gas in between the two chunks), then the (pressure, temperature) estimated from the two chunks of gas must (approximately) be a function of that latent. And, if there is some other latent about which the two chunks give the same information (like, say, a bit which is 1 if-and-only-if temperature is above 50 °C), then (pressure, temperature) estimated from the two chunks of gas must (approximately) also give that same information.

# General Case

Now we move on to more-than-two variables. The proofs generally follow the same structure as the two-variable case, just with more bells and whistles, and are mildly harder to intuit. This time, rather than ease into it, we’ll include approximation and other parts of the world () in the theorems upfront.

## The Fundamental Theorem

Suppose we have:

A distribution over random variables , …, ,

A latent variable which induces independence between all (first diagram below)

A latent variable which is insensitive to any given all the others (second diagram below)

Further, assume that mediates between and (third diagram below). This last assumption will be exactly satisfied by construction in the minimality/maximality theorems below.

Then, claim: mediates between and .

The diagrammatic proof, with approximation:

Note that the error bound is somewhat unimpressive, since it scales with the system size. We can strengthen the approximation mainly by using a stronger insensitivity condition for - for instance, if is insensitive to either of two *halves* of the system, then we can reuse the error bounds from the simplified 2-variable case earlier.

## Natural Latents

Suppose a single latent (approximately) satisfies both the main conditions

We call these the “naturality conditions”, and we call a (approximate) “natural latent” over .

The resample step works exactly as before: we’ll generally assume that has been resampled conditional on , and try to indicate that with the phrase “resampled natural latent”.

### Minimality & Maximality

Assume is a resampled natural latent over . Take *any* other latent about which gives (approximately) the same information as for any :

By the fundamental theorem:

So is, in this sense, the “most informative” latent about which all give the same information:

All give (approximately) the same information about , and for any other latent such that all give (approximately) the same information about tells us (approximately) everything which does about (and possibly more). This is the “maximality condition”.

Flipping things around: take any other latent which (approximately) induces independence between components of . By the fundamental theorem:

So is, in this sense, the “least informative” latent which induces independence between components of :

(approximately) induces independence between components of , and for any other latent which (approximately) induces independence between components of , tells us (approximately) everything which does about (and possibly more). This is the “minimality condition”.

Much like the simplified 2-variable case:

The minimality condition implies the natural latent conditions. Proof: take to be , for each .

Both minimality and maximality imply an approximately unique standard form (see appendix), so any natural latent in standard form is also the approximately unique natural and minimal and maximal latent in standard form. Furthermore, any natural latent can be transformed into standard form (as the phrase “standard form” implies).

In standard form, a natural latent is always approximately a deterministic function of . Specifically: .

Natural and minimal latents do not always exist, and maximal latents sometimes exist in cases where natural/minimal latents don’t.

Everything about approximation and other parts of the world carries over to naturality/minimality/maximality.

### Example

Suppose we have a die of unknown bias, which is rolled many times—enough to obtain a precise estimate of the bias many times over. Then, the die-rolls are independent given the bias, and we can get approximately-the-same estimate of the bias while ignoring any one die roll. So, the die’s bias is an approximate natural latent. The resampled natural latent is the bias sampled from a posterior distribution of the bias given the die rolls.

One interesting thing to note in this example: imagine that, instead of resampling the bias given the die rolls, we use the average frequencies from the die rolls. Would that be a natural latent? Answer in spoiler text:

The average frequencies tell us the exact counts of each outcome among the die rolls. So, with the average frequencies and all but one die roll, we can back out the value of that last die roll with certainty: just count up outcomes among all the other die rolls, then see which outcome is “missing”. That means the average frequencies and together give us much more information about than either one alone; neither of the two natural latent conditions holds.

This example illustrates that the “small” uncertainty in is actually load-bearing in typical problems. In this case, the low-order bits of the average frequencies contain lots of information relevant to , while the low-order bits of the natural latent don’t.

The most subtle challenges and mistakes in using natural latents tend to hinge on this point.

## Other Threads

We’ve now covered the main theorems of interest. This section offers a couple of conjectures, with minimal commentary.

### Universal Natural Latent Conjecture

Suppose there exists an approximate natural latent over . Construct a new random variable sampled from the distribution . (In other words: simultaneously resample each given all the others.) Conjecture: is an approximate natural latent (though the approximation may not be the best possible). And if so, a key question is: how good is the approximation?

Further conjecture: a natural latent exists over if-and-only-if is a natural latent over .(Note that we can always construct , regardless of whether a natural latent exists, and will always exactly satisfy the first natural latent condition over by construction.) Again, assuming the conjecture holds at all, a key question is to find the relevant approximation bounds.

### Maxent Conjecture

Assuming the universal natural latent conjecture holds, whenever there exists a natural latent and would approximately satisfy both of these two diagrams:

If we forget about all the context and just look at these two diagrams, one natural move is:

Convert to undirected graphical models (in this case, just remove the arrowheads)

Apply the Hammersley-Clifford method

… and the result would be that must be of the maxent form

for some .

Unfortunately, Hammersley-Clifford requires everywhere. Probabilities of zero are extremely load-bearing for natural latents in the exact case, and probabilities near zero are load-bearing in the approximate case; if the distribution is zero nowhere, then it can only have a natural latent if the ’s are all independent (in which case the trivial variable is a natural latent).

On the other hand, maxent sure does seem to be a theme of natural latents in e.g. physics. So the question is: does some version of this argument work? If there are loopholes, are there relatively few qualitative categories of loopholes which could be classified?

# Appendix: Machinery For Latent Variables

If you get confused about things like “what exactly is a latent variable?”, this is the appendix for you.

For our purposes, a latent variable over a random variable is *defined by* a distribution function - i.e. a distribution which tells us how to sample from . For instance, in the ideal gas example, the latent “average temperature” () can be defined by the distribution of average energy as a function of the gas state () - in this case a deterministic distribution, since average energy is a deterministic function of the gas state. As another example, consider the unknown bias of a die () and a bunch of rolls of the die (). We would take the latent bias to be *defined by* the function mapping the rolls to the posterior distribution of the bias given the rolls .

So, if we talk about e.g. “existence of a latent with the following properties …”, we’re really talking about the existence of a conditional distribution function , such that the random variable which it introduces satisfies the relevant properties. When we talk about “any latent satisfying the following properties …”, we’re really talking about any conditional distribution function such that the variable satisfies the relevant properties.

Toy mental model behind this way of treating latent variables: there are some variables out in the world, and those variables have some “true frequencies” . Different agents learn to model those true frequencies using different generative models, and those different generative models each contain their own latents. So the underlying distribution is fixed, but different agents introduce different latents with different ; is taken to be definitional because it tells us everything about the joint distribution of and which is not already pinned down by . (This is probably not the most general/powerful mental model to use for this math, but it’s a convenient starting point.)

## Standard Form of a Latent Variable

Suppose that consists of a bunch of rolls of a biased die, and a latent consists of the bias of the die along with the flip of one coin which is completely independent of the rest of the system. A different latent for the same system consists of just the bias of the die. We’d like some way to say that these two latents contain the same information *for purposes of *.

To do that, we’ll introduce a “standard form” (relative to ) for any latent variable :

We’ll say that a latent is “in standard form” if, when we use the above function to put it into standard form, we end up with a random variable equal to the original. So, a latent in standard form satisfies

As the phrase “standard form” suggests, putting a standard form latent into standard form leaves it unchanged, i.e. will satisfy for any latent ; that’s a lemma of the minimal map theorem.

Conceptually: the standard form throws out all information which is completely independent of , and keeps everything else. In standard statistics jargon: the likelihood function is always a minimal sufficient statistic. (See the minimal map theorem for more explanation.)

- The Plan − 2023 Version by 29 Dec 2023 23:34 UTC; 142 points) (
- 15 Feb 2024 0:03 UTC; 11 points) 's comment on Containment Thread on the Motivation and Political Context for My Philosophy of Language Agenda by (

It is a truth universally acknowledged that any article about the hidden nature of reality will not garner close to the number of comments as one about your sexy sexy homies. As the inaugural and possibly lone commenter, let me say I’m delighted to see finally this long-awaited post. I look forward to do a deep dive soon.

There’s a thing I keep thinking of when it comes to natural latents. In social science one often speaks of statistical sex differences, e.g. women tend to be nicer than men. But these sex differences aren’t deterministic, so one can’t derive them from simply meeting 1 woman and 1 man. It feels like this is in tension with the insensitivity condition, like that this only permits universal generalizations (I guess stuff like anatomy?). But also I haven’t really practiced natural latents at all so I sort of expect to be using them in a suboptimal way. Maybe you have a better idea?

Like I mean obviously one can deterministically recover it when one considers large samples of people, so it seems like maybe the “statistical man” and “statistical woman” concepts are different from the “universal man” and “universal woman” concepts. Not entirely sure this is a good approach though.

Quite the opposite! In that example, what the insensitivity condition would say is: if I get a big sample of people (roughly

^{50}⁄_{50}male/female), and quantify the average niceness of men and women in that sample, then I expect to get roughly the same numbers if I drop any one person (either man or woman) from the sample. It’s the statistical average which has to be insensitive; any one “sample” can vary a lot.That said, it does need to be more like a universal generalization

ifwe impose a stronger invariance condition. The strongest invariance condition would say that we can recover the latent from any one “sample”, which would be the sort of “universal generalization” you’re imagining. Mathematically, the main thing that would give us is much stronger approximations, i.e. smaller ϵ’s.Oops, my bad for focusing on the simplified version and then extrapolating incorrectly.

Let’s say every day at the office, we get three boxes of donuts, numbered 1, 2, and 3. I grab a donut from each box, plunk them down on napkins helpfully labeled X1, X2, and X3. The donuts vary in two aspects: size (big or small) and flavor (vanilla or chocolate). Across all boxes, the ratio of big to small donuts remains consistent. However, Boxes 1 and 2 share the same vanilla-to-chocolate ratio, which is different from that of Box 3.

Does the correlation between X1 and X2 imply that there is no natural latent? Is this the desired behavior of natural latents, despite the presence of the common size ratio? (and the commonality that I’ve only ever pulled out donuts; there has never been a tennis ball in any of the boxes!)

If so, why is this what we want from natural latents? If not, how does a natural latent arise despite the internal correlation?

My take would be to split each “donut” variable Xi into “donut size” Si and “donut flavour” Fi. Then there a natural latent for the whole {Si} set of variables, and no natural latent for the whole {Fi} set.{Fi} basically becomes the “other stuff in the world” Z variable relative to {Si}.

Granted, there’s an issue in that we can basically do that for any set of variables Xi, even entirely unrelated ones: deliberately search for some decomposition of Xi into an Si and an Fi such that there’s a natural latent for Si. I think some more practical measures could be taken into account here, though, to enure that the abstractions we find are useful. For example, we can check the relative information contents/entropies of {Xi} and {Si}, thereby measuring “how much” of the initial variable-set we’re abstracting over. If it’s too little, that’s not a useful abstraction.

^{[1]}That passes my common-sense check, at least. It’s essentially how we’re able to decompose and group objects along many different dimensions. We can focus on objects’ geometry (and therefore group all sphere-like objects, from billiard balls to planets to weather balloons) or their material (grouping all objects made out of rock) or their origin (grouping all man-made objects), etc.

Each grouping then corresponds to an abstraction, with its own generally-applicable properties. E. g., deriving a “sphere” abstraction lets us discover properties like “volume as a function of radius”, and then we can usefully apply that to any spherical object we discover. Similarly, man-made objects tend to have a purpose/function (unlike natural ones), which likewise lets us usefully reason about that whole category in the abstract.

(

Edit:On second thoughts, I think the obvious naive way of doing that just results in {Si} containing all mutual information between Xi, with the “abstraction” then just being said mutual information. Which doesn’t seem very useful. I still think there’s something in that direction, but probably not exactly this.)Relevant: Finite Factored Sets, which IIRC offer some machinery for these sorts of decompositions of variables.

This branch of research is aimed at finding a (nearly) objective way of thinking about the universe. When I imagine the end result, I imagine something that receives a distribution across a bunch of data, and finds a bunch of useful patterns within it. At the moment that looks like finding patterns in data via

`find_natural_latent(get_chunks_of_data(data_distribution))`

or perhaps showing that

`find_top_n(n, (chunks, natural_latent(chunks)) for chunks in`

`all_chunked_subsets_of_data(data_distribution),`

`key=lambda chunks, latent: usefulness_metric(latent))`

is a (convergent sub)goal of agents. As such, the notion that the donuts’ data is simply poorly chunked—which needs to be solved anyway—makes a lot of sense to me.

I don’t know how to think about the possibilities when it comes to decomposing Xi. Why would it always be possible to decompose random variables to allow for a natural latent? Do you have an easy example of this?

Also, what do you mean by mutual information between Xi, given that there are at least 3 of them? And why would just extracting said mutual information be useless?

If you get the chance to point me towards good resources about any of these questions, that would be great.

Regarding chunking: a background assumption for me is that the causal structure of the world yields a natural chunking, with each chunk taking up a little local “voxel” of spacetime.

Some amount spacetime-induced chunking is “forced upon” an embedded agent, in some sense, since their sensors and actuators are localized in spacetime.

Now, there’s still degrees of freedom in taking more or less coarse-grained chunkings, and more or less coarse-graining differentially along different spacetime directions or in different places. But I expect that spacetime locality mostly nails down what we need as a starting point for convergent chunking.

You can generalize mutual information to N variables: interaction information.

Well, I suppose I overstated it a bit by saying “always”; you can certainly imagine artificial setups where the mutual information between a bunch of variables is zero. In practice, however, everything in the world is correlated with everything else, so in a real-world setting you’ll likely find such a decomposition always, or almost always.

Well, not

uselessas such – it’s a useful formalism – but it would basically skip everything John and David’s post is describing. Crucially,it won’t uniquely determine whether a specific set of objects represents a well-abstracting category.The abstraction-finding algorithm should be able to successfully abstract over data if

and only ifthe underlying data actually correspond to some abstraction. If it can abstract over anything, however – any arbitrary bunch of objects – then whatever it is doing, it’s not finding “abstractions”. It may still be useful, but it’s not what we’re looking for here.Concrete example: if we feed our algorithm 1000 examples of trees, it should output the “tree” abstraction. If we feed our algorithm 200 examples each of car tires, trees, hydrogen atoms, wallpapers, and continental-philosophy papers, it shouldn’t actually find some abstraction which all of these objects are instances of. But as per the everything-is-correlated argument above, they likely have non-zero mutual information, so the naive “find a decomposition for which there’s a natural latent” algorithm would

fail to output nothing.More broadly: We’re looking for a “true name” of abstractions, and mutual information is sort-of related, but also clearly not precisely it.

I don’t understand how this is less information than a bit indicating whether the temperature is above 50C. Specifically, given a bit telling you whether the temperature is above 50C, how do you know whether the temperature is above 100C or between 50C and 100C?

Y’know, in hindsight I didn’t think that one through correctly when writing the example.

I know very, very little about category theory, but some of this work regarding natural latents seem to absolutely smack of it. There seems to be a fairly important three-way relationship between causal models, finite factored sets, and Bayes nets.

To be precise, any causal model consisting of root sets B, downstream sets X, and functions mapping sets to downstream sets like f4:(B1⊗B3⊗X2)→X4 must, when equipped with a set of independent probability distributions over B, create a joint probability distribution compatible with the Bayes net that’s isomorphic to the causal model in the obvious way. (So in the previous example, there would be arrows from only B1, B3, and X2 to X4) The proof of this seems almost trivial but I don’t trust myself not to balls it up somehow when working with probability theory notation.

In the resulting Bayes net, one “minimal” natural latent which conditionally separates Xi and Xj is just the probabilities over just the root elements from B which both Xi and Xj depend on. It might be possible to show that this “minimal” construction of Λ satisfies a universal property, and so other Λ′ which is also “minimal” in this way must be isomorphic to Λ.

Absent feedback, today I read further, to the premise of the maxent conjecture. Let X be 100 numbers up to 1 million, rerolled until the remainder of their sum modulo 1000000 ends up 0 or 1. (X’ will have sum-remainder circa 50 or circa −50.) Given X’, X1 has a 25%/50%/25% pattern around X′1. Given X2 through X100, X1 has a 50%/50% distribution. So the (First/Strong) Universal Natural Latent Conjecture fails, right?

I believe no natural latent exists in that case?

The Universal Natural Latent Conjecture doesn’t say X’ is always a natural latent, it says X’ is a natural latent

ifany natural latent exists.One thing that initially stood out to me on the fundamental theorem was: where did the N→M arrow come from? It ‘gets introduced’ in the first bookkeeping step (we draw N→M and then reorder the (N,M,X¯i) subgraph at each i.

This seemed suspicious to me at first! It seemed like kind of a choice, so what if we just didn’t add that arrow? Could we land at a conclusion of N AND M→X? That’s way too strong! But I played with it a bit, and there’s no obvious way to do the second frankenstitch which brings everything together

unlessyou draw in that extra arrow and rearrange. You just can’t get a globally consistent topological ordering without N somehow becoming ancesterable to X¯i. (Otherwise the glommed X¯i variables interfere with each other when you try to find N’s ancestors in the stitch.)Still, this move seems quite salient—in particular that arrow-addition feels something like the ‘lossiest’ step in the proof (except for the final bookkeeping which gloms all the Xi together, implicitly drawing a load of arrows between them all)?

Is my understanding correct or am I missing something?

A latent variable is a variable you can sample that gives you some subset of the mutual information between all the different X’s + possibly some independent extra “noise” unrelated to the X’s

A natural latent is a variable that you can sample that at the limit of sampling will give you

allthe mutual information between the X’s—nothing more or lessE.g. in the biased die example, every each die roll sample has, in expectation, the same information content, which is the die bias + random noise, and so the mutual info of

nrolls is the die bias itself(where “different X’s” above can be thought of as different (or the same) distributions over the observation space of X corresponding to the different sampling instances, perhaps a non-standard framing)

First bullet is correct, second bullet is close but not quite right. Just one sample of a natural latent will give you (approximately) all the mutual information between the X’s, and can give you some additional “noise” as well.

E.g. in the biased die example with many rolls, we can sample the bias given the rolls. Because that distribution is very pointy the sample will be very close to the “true bias”, that one sample will capture approximately-all of the mutual information between the rolls.

(Note: I did skip a subtle step there—our natural latents need a stronger condition than just “close to the true bias” in this example, since the low-order bits of the latent could in-principle contain a bunch of relevant information which the true bias doesn’t; that would mess everything up. And indeed, that

wouldmess everything up if we tried to use e.g. the empirical frequencies rather than a sample from P[bias | X]: given all but one die roll and the empirical frequencies calculated from all of the die rolls, we could exactly calculate the outcome of the remaining die roll. That’s why we do the sampling thing; the little bit of noise introduced by sampling is load-bearing, since it wipes out info in those low-order bits.… but that’s a subtlety which you should not worry about until

afterthe main picture makes sense conceptually.)Speaking as an (ex-)scientist, the fact that natural latents exist, can be found, and are well defined and basically unique for a systems feels… blindingly obvious: we do this all the time. But I gather we never previously had a description of their necessary properties in term of Bayes nets before, nor a proof of in what sense they are unique. I don’t think I was ever very worried that AI was going to discover an entirely different ontology for physics so different that pressure or temperature were not well-defined abstractions represented in it, but I also didn’t have a uniqueness proof demonstrating that fact, and with the fate of the human race potentially on the line, that’s a reassuring thing to have. Physicists often have a tendency to take on trust things that any mathematician would be aghast at, just because they seem to work in practice. [But then, neither have I ever figured out why anyone thinks the diamond-maximization problem is hard, as opposed to just tedious (you just have to list your purity specifications in isotopic and crystalographic terms, and then put it inside a standard causal wrapper).]

Fix some atom of information. It’s contained in some of Lambda, X1, X2, and Lambda’. Call the corresponding four statements a,b,c,d. Then you assume “b&c implies a, c&d implies b, b&d implies c, a&d implies b or c.”.

These compress into “b&c implies a, d implies a=b=c.”; after concluding that, I read that you conclude “d&(b or c) implies a”, which seems to be a special case. My approach feels too gainfully simpler, so I’m checking in to ask whether it fails.

Just pasting this into a calculator your expressions don’t seem to be equivalent:

first expression e1: (((b∧c)=>a) ∧ ((c ∧ d) ⇒ b) ∧ (d ∧ b ⇒ c) ∧ ((a ∧ d) =>(b or c)))

second expression e2: ((b∧c)=>a)∧(d =>((a=b)=c))

e1 = e2: (a ∧ b) ∨ (a ∧ c) ∨ (b ∧ c) ∨ ¬ d

e1 simplifies to (a ∧ b ∧ c) ∨ (¬ a ∧ ¬ b ∧ ¬ c) ∨ (¬ b ∧ ¬ d) ∨ (¬ c ∧ ¬ d)

For e2 I think you want ((b∧c)=>a)∧(d =>((a=b)∧(a=c)))

Oops!

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