Consider the following program:

```
f(n):
if n == 0:
return 1
return n * f(n-1)
```

Let’s think about the process by which this function is evaluated. We want to sketch out a causal DAG showing all of the intermediate calculations and the connections between them (feel free to pause reading and try this yourself).

Here’s what the causal DAG looks like:

Each dotted box corresponds to one call to the function f. The recursive call in f becomes a symmetry in the causal diagram: the DAG consists of an infinite sequence of copies of the same subcircuit.

More generally, we can represent any Turing-computable function this way. Just take some pseudocode for the function, and expand out the full causal DAG of the calculation. In general, the diagram will either be finite or have symmetric components - the symmetry is what allows us to use a finite representation even though the graph itself is infinite.

## Why would we want to do this?

For our purposes, the central idea of embedded agency is to take these black-box systems which we call “agents”, and break open the black boxes to see what’s going on inside.

Causal DAGs with symmetry are how we do this for Turing-computable functions in general. They show the actual cause-and-effect process which computes the result; conceptually they represent the *computation* rather than a black-box *function*.

In particular, a causal DAG + symmetry representation gives us all the natural machinery of causality - most notably counterfactuals. We can ask questions like “what would happen if I reached in and flipped a bit at this point in the computation?” or “what value would f(5) return if f(3) were 11?”. We can pose these questions in a well-defined, unambiguous way without worrying about logical counterfactuals, and without adding any additional machinery. This becomes particularly important for embedded optimization: if an “agent” (e.g. an organism) wants to plan ahead to achieve an objective (e.g. find food), it needs to ask counterfactual questions like “how much food would I find if I kept going straight?”.

The other main reason we would want to represent functions as causal DAGs with symmetry is because our universe appears to be one giant causal DAG with symmetry.

Because our universe is causal, any computation performed in our universe must eventually bottom out in a causal DAG. We can write our programs in any language we please, but eventually they will be compiled down to machine code and run by physical transistors made of atoms which are themselves governed by a causal DAG. In most cases, we can represent the causal computational process at a more abstract level - e.g. in our example program, even though we didn’t talk about registers or transistors or electric fields, the causal diagram we sketched out would still accurately represent the computation performed even at the lower levels.

This raises the issue of abstraction - the core problem of embedded agency. My own main use-case for the causal diagram + symmetry model of computation is formulating models of abstraction: how can one causal diagram (possibly with symmetry) represent another in a way which makes counterfactual queries on the map correspond to some kind of counterfactual on the territory? Can that work when the “map” is a subDAG of the territory DAG? It feels like causal diagrams + symmetry are the minimal computational model needed to get agency-relevant answers to this sort of question.

## Learning

The traditional ultimate learning algorithm is Solomonoff Induction: take some black-box system which spews out data, and look for short programs which reproduce that data. But the phrase “black-box” suggests that perhaps we could do better by looking inside that box.

To make this a little bit more concrete: imagine I have some python program running on a server which responds to http requests. Solomonoff Induction would look at the data returned by requests to the program, and learn to predict the program’s behavior. But that sort of black-box interaction is not the only option. The program is running on a physical server somewhere - so, in principle, we could go grab a screwdriver and a tiny oscilloscope and directly observe the computation performed by the physical machine. Even without measuring every voltage on every wire, we may at least get enough data to narrow down the space of candidate programs in a way which Solomonoff Induction could not do. Ideally, we’d gain enough information to avoid needing to search over all possible programs.

Compared to Solomonoff Induction, this process looks a lot more like how scientists actually study the real world in practice: there’s lots of taking stuff apart and poking at it to see what makes it tick.

In general, though, how to learn causal DAGs with symmetry is still an open question. We’d like something like Solomonoff Induction, but which can account for partial information about the internal structure of the causal DAG, rather than just overall input-output behavior. (In principle, we could shoehorn this whole thing into traditional Solomonoff Induction by treating information about the internal DAG structure as normal old data, but that doesn’t give us a good way to extract the learned DAG structure.)

We already have algorithms for learning causal structure in general. Pearl’s Causality sketches out some such algorithms in chapter 2, although they’re only practical for either very small systems or very large amounts of data. Bayesian structure learning can handle larger systems with less data, though sometimes at the cost of a very large amount of compute - i.e. estimating high-dimensional integrals.

However, in general, these approaches don’t directly account for *symmetry* of the learned DAGs. Ideally, we would use a prior which weights causal DAGs according to the size of their representation - i.e. infinite DAGs would still have nonzero prior probability if they have some symmetry allowing for finite representation, and in general DAGs with multiple copies of the same sub-DAG would have higher probability. This isn’t quite the same as weighting by minimum description length in the Solomonoff sense, since we care specifically about symmetries which correspond to function calls - i.e. isomorphic subDAGs. We don’t care about graphs which can be generated by a short program but don’t have these sorts of symmetries. So that leaves the question: if our prior probability for a causal DAG is given by a notion of minimum description length which only allows compression by specifying re-used subcircuits, what properties will the resulting learning algorithm possess? Is it computable? What kinds of data are needed to make it tractable?

Thanks for a nice post about causal diagrams!

Totally agree. This is a big part of the reason why I'm excited about these kinds of diagrams.

Great question, I really think someone should look more carefully into this. A few potentially related papers:

https://arxiv.org/abs/1105.0158

https://arxiv.org/abs/1812.03789

Again, agreed. It would be great if we could find a way to make progress on this question.

A few comments:

Because of quantum physics, the universe is actually

notdescribed by a causal DAG very well (if we require microscopic precision). But I agree that in practice there are usefulapproximatedescriptions that do look like a causal DAG.One direction towards studying the learning of symmetric causal DAGs (of a sort) is my ideas about cellular decision processes and the more general "graph decision processes", see this comment.

As a side note, I'm not convinced that "breaking open black boxes" to solve "embedded agency" is a useful way of thinking. IMO the problems associated with "embedded agency" should be solved using a combination of incomplete models and correctly dealing with traps.

The quantum fields themselves follow causality just fine. Things only become weird if we introduce wave-function collapse, which isn't strictly necessary.

Hmm, no, not really. The quantum fields follow "causality" in some quantum sense (roughly speaking, operators in spacelike separations commute, and any local operator can be expressed in terms of operators localized near the intersection of its past light-cone with any spacelike hypersurface), which is different from the sense used in causal DAGsa (in fact you can define "quantum causal DAGs" which is a different mathematical object). Violation of Bell's inequality precisely means that you can't describe the system by a causal DAG. If you want to do the MWI, then the wavefunction doesn't even decompose into data that can be localized.

No, violation of Bell's inequality means you can't describe the system by causal interactions

among particles and measurements. If we stop thinking about particles and "measurements" altogether, and just talk about fields, that's not an issue.As you say, under MWI, the wavefunction doesn't even decompose into data that can be localized. So, in order to represent the system using classical causal diagrams, the "system state" has to contain the whole wavefunction. As long as we can write down an equation for the evolution of the wavefunction over time, we have a classical causal model for the system.

Quantum causal models are certainly a much cleaner representation, in this case, but classical causal models can still work - we just have to define the "DAG vertices" appropriately.

It doesn't really have much to do with particles vs. fields. We talk about measurements because measurements are the thing we actually observe. It seems strange to say you can model the world as a causal network if the causal network doesn't include your actual observations. If you want to choose a particular frame of reference and write down the wavefunction time evolution in that frame (while ignoring space) then you can say it's a causal network (which is just a linear chain, and deterministic at that) but IMO that's not very informative. It also loses the property of having things made of parts, which AFAIU was one of your objectives here.

The wavefunction does have plenty of internal structure, that structure just doesn't line up neatly with space. It won't just be a linear chain, and it will be made of "parts", but those parts won't necessarily line up neatly with macroscopic observations/objects.

And that's fine - figuring out how to do ontology mapping between the low-level "parts" and the high-level "parts" is a central piece of the problem. Not being able to directly observe variables in the low-level causal diagram is part of that. If we want e.g. a theory of abstraction, then these issues are perfect use-cases.

I really like this model of computation and how naturally it deals with counterfactuals, surprised it isn't talked about more often.

I'd like to understand this claim better - are you saying that the core problem of embedded agency is relating high-level agent models (represented as causal diagrams) to low-level physics models (also represented as causal diagrams)?

I'm saying that the core problem of embedded agency is relating a high-level, abstract map to the low-level territory it represents. How can we characterize the map-territory relationship based on our knowledge of the map-generating process, and what properties does the map-generating process need to have in order to produce "accurate" & useful maps? How do queries on the map correspond to queries on the territory? Exactly what information is kept and what information is thrown out when the map is smaller than the territory? Good answers to these question would likely solve the usual reflection/diagonalization problems, and also explain when and why world-models are needed for effective goal-seeking behavior.

When I think about how to formalize these sort of questions in a way useful for embedded agency, the minimum requirements are something like:

... and causal diagrams with symmetry seem like the natural class to capture all that.