## Computational Category Theory in Python III: Monoids, Groups, and Preorders

Parts 1 and 2 are found here and here

From one perspective, categories are just another algebraic structure, like groups, monoids and rings. They are these abstract things that have some abstract equational axioms and operations. They are the next stop on our magnificent category journey.

A monoid is a thing that has an associative operation with a unit. Addition and 0 make numbers a monoid. Multiplication and 1 are a separate monoid for numbers. Concatenation and empty lists make lists a monoid. Union and empty set make sets a monoid. We can encode this in python like so:

What does this have to do with categories? Well, if some thing is a category, it obeys the axioms that define what it means to be a category. It has morphisms and objects. The morphisms compose if head meets tail on an object. There are always identity morphism.

The morphisms in a category with 1 object automatically obey the monoid axioms. In this case, the category axioms imply the monoid axioms. Everything composes because there is only one object. It’s a kind of degenerate case where we are not using the partiality of the composition operator. There is automatically a unit for composition because the identity morphism is a unit. Composition is already required to be associative. Boom. The thing is a monoid.

Continuing with our representation from previous posts, we make a python class for each category. An instance of this class is a morphism in this category. If you ask for the domain or codomain of any morphism, you always get back () because it is a single object category. Compare these classes with the above classes.

Some monoids are also groups if there is a natural inverse operation. The integers are a group under addition where the negative gives you the inverse. Some aren’t though. The natural numbers (0,1,2…) aren’t a group under addition though.

Similarly groups can be thought of as a category with one object, with the additional requirement that every morphism is invertible, that there is always a $f^{-1}$ such that $f \circ f^{-1} = id$.

Sympy has groups in it. We can make a wrapper of that functionality that looks like a categorical interface. To match our pattern of using python classes to represent categories, it is convenient to do the slightly uncommon thing of making a class definition generator function fp_group_cat. Every time you call this function, it makes a different class and a different category. I have only here wrapped the finitely presented group functionality, but there are also free groups, permutation groups, and named groups available in sympy.

#### Many objects, at most one arrow per pair: Preorders

We can simplify the power of a category in a different direction. Instead of having only 1 object, we’ll have few arrows.

A category with many objects but at most a single morphism between a pair of them obeys the axioms of a preorder. In categorical terminology this is sometimes called a thin category Any actual order like like $\le$ on numbers is also a preorder, but preorders have slightly weaker requirements. Here is a categorical representation of the ordering on integers (although really the same implementation will work for any python type that implements <= and == )

An example of a partial order is the subset relationship, which we can represent using python sets. This is an important but perhaps confusing example. Haven’t we already defined FinSet? Yes, but these are different categories. In FinSet, morphisms are functions. In SubSetCat a morphisms is the subset relationship (of which there can either be one or not one). They just plain are not the same thing even though there are sets in the mix for both. The situation is made even more confusing by the fact that the subset relationship can be talked about indirectly inside FinSet using monic morphisms, which have as their image the subset of interest.

Preorders are related to directed acyclic graphs (DAG), the directed graphs that have no loops. If you give me a DAG, there is a preorder that is generated by that DAG. Exercise for the reader (AKA I’m lazy): Can you turn a Networkx DAG into a category?

### Thoughts

This is nice and all just to explain categories in terms of some perhaps more familiar concepts. It feels a little ho-hum to me. We are not getting really any benefit from the concept of a category from this post. However, the examples of monoids, groups and preorders are always something you should think about when presented when a new categorical concept, because it probably reduces to something more familiar in this case. In addition, mappings to/from these simple objects to more complicated categories can be very interesting.

The methods of computational group theory are intriguing. It seems like some of them should extend to category theory. See this book by RFC Walters for example https://www.cambridge.org/core/books/categories-and-computer-science/203EBBEE29BEADB035C9DD80191E67B1 A very interesting book in other ways too. (Thanks to Evan Patterson for the tip)

Next time I think we’ll talk about finite categories and the finite Yoneda lemma.

Artwork courtesy of David

Edit: Hacker News discussion: https://news.ycombinator.com/item?id=23058551

## Computational Category Theory in Python II: Numpy for FinVect

Linear algebra seems to be the place where any energy you put in to learning it seems to pay off massively in understanding other subjects and applications. It is the beating heart of numerical computing. I can’t find the words to overstate the importance of linear algebra.

Here’s some examples:

• Least Squares Fitting – Goddamn is this one useful.
• Partial Differential Equations – Heat equations, electricity and magnetism, elasticity, fluid flow. Differential equations can be approximated as finite difference matrices acting on vectors representing the functions you’re solving for.
• Linear Dynamical systems – Solving, frequency analysis, control, estimation, stability
• Signals – Filtering, Fourier transforms
• Quantum mechanics – Eigenvalues for energy, evolving in time, perturbation theory
• Probability – Transition matrices, eigenvectors for steady state distributions.
• Multidimensional Gaussian integrals – A canonical model in quantum mechanics and probability because they are solvable in closed form. Gaussian integrals are linear algebra in disguise. Their solution is describable in terms of the matrices and vectors in the exponent. More on this another day.

Where does category theory come in to this?

On one side, exploring what categorical constructions mean concretely and computationally in linear algebra land helps explain the category theory. I personally feel very comfortable with linear algebra. Matrices make me feel good and safe and warm and fuzzy. You may or may not feel the same way depending on your background.

In particular, understanding what the categorical notion of a pullback means in the context of matrices is the first time the concept clicked for me thanks to discussions with James Fairbanks and Evan Patterson.

But the other direction is important too. A categorical interface to numpy has the promise of making certain problems easier to express and solve. It gives new tools for thought and programming. The thing that seems the most enticing to me about the categorical approach to linear algebra is that it gives you a flexible language to discuss gluing together rectangular subpieces of a numerical linear algebra problem and it gives a high level algebra for manipulating this gluing. Down this road seems to be an actionable, applicable, computational, constructible example of open systems.

Given how important linear algebra is, given that I’ve been tinkering and solving problems (PDEs, fitting problems, control problems, boundary value problems, probabilistic dynamics, yada yada ) using numpy/scipy for 10 years now and given that I actually have a natural reluctance towards inscrutable mathematics for its own sake, I hope that lends some credence to when I say that there really is something here with this category theory business.

It frankly boggles my mind that these implementations aren’t available somewhere already! GAH!

Uh oh. I’m foaming. I need to take my pills now.

### FinVect

The objects in the category FinVect are the vector spaces. We can represent a vector space by its dimensionality n (an integer). The morphisms are linear maps which are represented by numpy matrices. ndarray.shape basically tells you what are the domain and codomain of the morphism. We can get a lot of mileage by subclassing ndarray to make our FinVect morphisms. Composition is matrix multiplication (which is associative) and identity morphisms are identity matrices. We’ve checked our category theory boxes.

A part of the flavor of category theory comes from taking the focus away from the objects and putting focus on the morphisms.

One does not typically speak of the elements of a set, or subsets of a set in category theory. One takes the slight indirection of using the map whose image is that subset or the element in question when/if you need to talk about such things.

This actually makes a lot of sense from the perspective of numerical linear algebra. Matrices are concrete representations of linear maps. But also sometimes we use them as data structures for collections of vectors. When one wants to describe a vector subspace concretely, you can describe it either as the range of a matrix or the nullspace of a matrix. This is indeed describing a subset in terms of a mapping. In the case of the range, we are describing the subspace as all possible linear combinations of the columns $\lambda_1 c_1 + \lambda_2 c_2 + ...$ . It is a matrix mapping from the space of parameters $\lambda$ to the subspace (1 dimension for each generator vector / column). In the case of the nullspace it is a matrix mapping from the subspace to the space of constraints (1 dimension for each equation / row).

The injectivity or surjectivity of a matrix is easily detectable as a question about its rank. These kinds of morphisms are called monomorphisms and epimorphisms respectively. They are characterized by whether you can “divide” out by the morphism on the left or on the right. In linear algebra terms, whether there is a left or right inverse to these possibly rectangular, possibly ill-posed matrices. I personally can never remember which is which (surf/ing, left/right, mono/epi) without careful thought, but then again I’m an ape.

Some categorical constructions are very simple structural transformation that correspond to merely stacking matrices, shuffling elements, or taking transposes. The product and coproduct are examples of this. The product is an operation that takes in 2 objects and returns a new object, two projections $\pi_1$ $\pi_2$ and a function implementing the universal property that constructs $f$ from $f_1 f_2$.

Here is the corresponding python program. The matrix e (called f in the diagram. Sorry about mixed conventions. ) is the unique morphism that makes those triangles commute, which is checked numerically in the assert statements.

The coproduct proceeds very similarly. Give it a shot. The coproduct is more similar to the product in FinVect than it is in FinSet.

The initial and terminal objects are 0 dimensional vector spaces. Again, these are more similar to each other in FinVect than they are in FinSet. A matrix with one dimension as 0 really is unique. You have no choice for entries.

Where the real meat and potatoes lives is in the pullback, pushout, equalizer, and co-equalizer. These are the categorical constructions that hold equation solving capabilities. There is a really nice explanation of the concept of a pullback and the other above constructions here .

Vector subspaces can be described as the range of the matrix or the nullspace of a matrix. These representations are dual to each other in some sense. $RN=0$. Converting from one representation to the other is a nontrivial operation.

In addition to thinking of these constructions as solving equations, you can also think of a pullback/equalizer as converting a nullspace representation of a subspace into a range representation of a subspace and the coequalizer/pushout as converting the range representation into a nullspace representation.

The actual heart of the computation lies in the scipy routine null_space and orth. Under the hood these use an SVD decomposition, which seems like the most reasonable numerical approach to questions about nullspaces. (An aside: nullspaces are not a very numerical question. The dimensionality of a nullspace of a collection of vectors is pretty sensitive to perturbations. This may or may not be an issue. Not sure. )

Let’s talk about how to implement the pullback. The input is the two morphisms f and g. The output is an object P, two projections p1 p2, and a universal property function that given q1 q2 constructs u. This all seems very similar to the product. The extra feature is that the squares are required to commute, which corresponds to the equation $f p_1 = g p_2$ and is checked in assert statements in the code. This is the equation that is being solved. Computationally this is done by embedding this equation into a nullspace calculation $\begin{bmatrix} F & -G \end{bmatrix} \begin{bmatrix} x \\ y \end{bmatrix} = 0$. The universal morphism is calculated by projecting q1 and q2 onto the calculated orthogonal basis for the nullspace. Because q1 and q2 are required to be in a commuting square with f and g by hypothesis, their columns live in the nullspace of the FG stacked matrix. There is extra discussion with James and Evan and some nice derivations as mentioned before here

The equalizer, coequalizer, and pushout can all be calculated similarly. A nice exercise for the reader (AKA I’m lazy)!

## Thoughts

I think there are already some things here for you to chew on. Certainly a lot of polish and filling out of the combinators is required.

I am acutely aware that I haven’t shown any of this being used. So I’ve only shown the side where the construction helps teach us category theory and not entirely fulfilled the lofty promises I set in the intro. I only have finite endurance. I’m sure the other direction, where this helps us formulate problems, will show up on this blog at some point. For what I’m thinking, it will be something like this post http://www.philipzucker.com/linear-relation-algebra-of-circuits-with-hmatrix/ but in a different pullback-y style. Mix together FinSet and FinVect. Something something decorated cospans? https://arxiv.org/abs/1609.05382

One important thing is we really need to extend this to affine maps rather than linear maps (affine maps allow an offset $y = Ax + b$. This is important for applications. The canonical linear algebra problem is $Ax=b$ which we haven’t yet shown how to represent.

One common approach to embed the affine case in the linear case is to use homogenous coordinates. https://en.wikipedia.org/wiki/Homogeneous_coordinates.

Alternatively, we could make a new python class FinAff that just holds the b vector as a separate field. Which approach will be more elegant is not clear to me at the moment.

Another very enticing implementation on the horizon is a nice wrapper for compositionally calculating gaussian integrals + linear delta functions. Gaussian integrals + delta functions are solved by basically a minimization problem over the exponent. I believe this can be formulated by describing the linear subspace we are in as a span over the input and output variables, associating a quadratic form with the vertex of the span. You’ll see.

### Blah Blah Blah

Whenever I write a post, I just let it flow, because I am entranced by the sound of my own keyboard clackin’. But it would deeply surprise me if you are as equally entranced, so I take sections out that are just musings and not really on the main point. So let’s toss em down here if you’re interested.

I like to draw little schematic matrices sometimes so I can visually see with dimensions match with which dimensions.

Making the objects just the dimension is a structural approach and you could make other choices. It may also make sense to not necessarily identify two vector spaces of the same dimensionality. It is nonsensical to consider a vector of dog’s nose qualities to be interchangeable with a vector of rocket ship just because they both have dimensionality 7.

#### High Level Linear Algebra

Linear algebra already has some powerful high level abstractions in common use.

Numpy indexing and broadcasting can sometimes be a little cryptic, but it is also very, very powerful. You gain both concision and speed.

Matrix notation is the most commonly used “pointfree” notation in the world. Indexful expressions can be very useful, but the calculus of matrices lets us use intuition built about algebraic manipulation of ordinary numbers to manipulate large systems of equations in a high level way. There are simple rules governing matrix inverse, transpose, addition, multiplication, identity.

Another powerful notion in linear algebra is that of block matrices. Block matrices are the standard high level notation to talk about subpieces of a numerical linear algebra problem. For example, you might be solving the heat equation on two hunks of metal attached at a joint. It is natural to consider this system in block form with the off diagonal blocks corresponding to the coupling of the two hunks. https://en.wikipedia.org/wiki/Domain_decomposition_methods

One does not typically speak of the elements of a set, or subsets of a set in category theory. One takes the slight indirection of using the map whose image is that subset or the element in question when/if you need to talk about such things. This pays off in a couple ways. There is a nice minimalism in that you don’t need a whole new entity (python class, data structure, what have you) when you already have morphisms lying around. More importantly though the algebraic properties of what it means to be an element or subset are more clearly stated and manipulated in this form. On the flipside, given that we often return to subset or element based thinking when we’re confused or explaining something to a beginner shows that I think it is a somewhat difficult game to play.

The analogy is that a beginner will often write for loops for a numpy calculation that an expert knows how to write more concisely and efficiently using broadcasting and vectorization. And sometimes the expert just can’t figure out how to vectorize some complicated construction and defeatedly writes the dirty feeling for loop.

What about in a language where the for loops are fast, like Julia? Then isn’t the for loop version just plain better, since any beginner can read and write it and it runs fast too? Yes, I think learning some high level notation or interface is a harder sell here. Nevertheless, there is utility. High level formulations enable optimizing compilers to do fancier things. They open up opportunities for parallelism. They aid reasoning about code. See query optimization for databases. Succinctness is surprising virtue in and of itself.

Aaron Hsu (who is an APL beast) said something that has stuck with me. APL has a reputation for being incredibly unscrutable. It uses characters you can’t type, each of which is a complex operation on arrays. It is the epitome of concision. A single word in APL is an entire subroutine. A single sentence is a program. He says that being able to fit your entire huge program on a single screen puts you in a different domain of memory and mindspace. That it is worth the inscrutability because once trained, you can hold everything in your extended mind at once. Sometimes I feel when I’m writing stuff down on paper that it is an extension of my mind, that it is part of my short term memory. So too the computer screen. I’m not on board for APL yet, but food for thought ya know?

#### Differences between the pure mathematical perspective of Linear Algebra, and the Applied/Numerical Linear Alegbra

I think there a couple conceptual points of disconnect between the purely mathematical conception of vector spaces and the applied numerical perspective.

First off, the numerical world is by and large focused on full rank square matrices. The canonical problem is solving the matrix equation $Ax=b$ for the unknown vector x. If the matrix isn’t full rank or square, we find some way to make it square and full rank.

The mathematical world is more fixated on the concept of a vector subspace, which is a set of vectors.

It is actually extremely remarkable and I invite you for a moment to contemplate that a vector subspace over the real numbers is a very very big set. Completely infinite. And yet it is tractable because it is generated by only a finite number of vectors, which we can concretely manipulate.

Ok. Here’s another thing. I am perfectly willing to pretend unless I’m being extra careful that machine floats are real numbers. This makes some mathematicians vomit blood. I’ve seen it. Cody gave me quite a look. Floats upon closer inspection are not at all the mathematical real numbers though. They’re countable first off.

From a mathematical perspective, many people are interested in precise vector arithmetic, which requires going to somewhat unusual fields. Finite fields are discrete mathematical objects that just so happen to actually have a division operation like the rationals or reals. Quite the miracle. In pure mathematics they more often do linear algebra over these things rather than the rationals or reals.

The finite basis theorem. This was brought up in conversation as a basic result in linear algebra. I’m not sure I’d ever even heard of it. It is so far from my conceptualization of these things.

### Monoidal Products

The direct sum of matrices is represented by taking the block diagonal. It is a monoidal product on FinVect. Monoidal products are binary operations on morphisms in a category that play nice with it in certain ways. For example, the direct sum of two identity matrices is also an identity matrix.

The kronecker product is another useful piece of FinVect. It is a second monoidal product on the catgeory FinVect It is useful for probability and quantum mechanics. When you take the pair of the pieces of state to make a combined state, you

    def par(f,g):
''' One choice of monoidal product is the direct sum '''
r, c = f.shape
rg, cg = g.shape
return Vect(np.block( [ [f       ,           np.zeros((r,cg))]  ,
[np.zeros((rg,c))  , g              ]]  ))
def par2(f,g):
'''  another choice is the kroncker product'''
return np.kron(f,g)

We think about row vectors as being matrices where the number of columns is 1 or column vectors as being matrices where the number of rows is 1. This can be considered as a mapping from/to the 1 dimensional vector. These morphisms are points.

The traditional focus of category theory in linear algebra has been on the kronecker product, string diagrams as quantum circuits/ penrose notation, and applications to quantum mechanics.

However, the direct sum structure and the limit/co-limit structures of FinVect are very interesting and more applicable to everyday engineering. I associate bringing more focus to this angle with John Baez’s group and his collaborators.

Anyway, that is enough blithering.

## Computational Category Theory in Python I: Dictionaries for FinSet

Category theory is a mathematical theory with reputation for being very abstract.

Category theory is an algebraic theory of functions. It has the flavor of connecting up little pipes and ports that is reminiscent of dataflow languages or circuits, but with some hearty mathematical underpinnings.

So is this really applicable to programming at all? Yes, I think so.

Here’s one argument. Libraries present an interface to their users. One of the measures of the goodness or badness of an interface is how often you are inclined to peek under the hood to get it to do the thing that you need. Designing these interfaces is hard. Category theory has taken off as a field because it has been found to be a useful and uniform interface to a surprising variety of very different mathematics. I submit that it is at least plausible that software interfaces designed with tasteful mimicry of category theory may achieve similar uniformity across disparate software domains. This is epitomized for me in Conal Elliott’s Compiling to Categories. http://conal.net/papers/compiling-to-categories/

I think it is easy to have the miscomprehension that a fancy language like Haskell or Agda is necessary to even begin writing software that encapsulates category theory based ideas, but this is simply not the case. I’ve been under this misapprehension before.

It just so happens that category theory is especially useful in those languages for explaining some programming patterns especially those concerning polymorphism. See Bartosz Milewski’s Category theory for Programmers.

But this is not the only way to use category theory.

There’s a really delightful book by Rydeheard and Burstall called Computational Category Theory. The first time I looked at it, I couldn’t make heads or tails of it, going on the double uphill battle of category theory and Standard ML. But looking at it now, it seems extremely straightforward and well presented. It’s a cookbook of how to build category theoretic interfaces for software.

So I think it is interesting to perform some translation of its concepts and style into python, the lingua franca of computing today.

In particular, there is a dual opportunity to both build a unified interface between some of the most commonly used powerful libraries in the python ecosystem and also use these implementations to help explain categorical concepts in concrete detail. I hope to have the attention span to do this following:

A very simple category is that of finite sets. The objects in the category can be represented by python sets. The morphisms can be represented by python dictionaries. Nothing abstract here. We can rip and tear these things apart any which way we please.

The manipulations are made even more pleasant by the python features of set and dictionary comprehension which will mimic the definitions you’ll find on the wikipedia page for these constructions quite nicely.

Composition is defined as making a new dictionary by feeding the output of the first dictionary into the second. The identity dictionary over a set is one that has the same values as keys. The definition of products and coproducts (disjoint union) are probably not too surprising.

One really interesting thing about the Rydeheard and Burstall presentation is noticing what are the inputs to these constructions and what are the outputs. Do you need to hand it objects? morphisms? How many? How can we represent the universal property? We do so by outputting functions that construct the required universal morphisms. They describe this is a kind of skolemization . The constructive programmatic presentation of the things is incredibly helpful to my understanding, and I hope it is to yours as well.

Here is a python class for FinSet. I’ve implemented a couple of interesting constructions, such as pullbacks and detecting monomorphisms and epimorphisms.

I’m launching you into the a deep end here if you have never seen category theory before (although goddamn does it get deeper). Do not be surprised if this doesn’t make that much sense. Try reading Rydeheard and Burstall chapter 3 and 4 first or other resources.

Here’s some fun exercises (Ok. Truth time. It’s because I got lazy). Try to implement exponential and pushout for this category.

## Uniform Continuity is Kind of Like a Lens

A really interesting topic is exact real arithmetic. It turns out, there are systematic ways of calculating numerical results with arbitrarily fine accuracy.

In practice this is not used much as it is complicated and slow.

There are deep waters here.

The problem is made rather difficult by the fact that you can’t compute real numbers strictly, you have to in some sense compute better and better finite approximations.

One way of doing this is to compute a stream of arbitrarily good approximations. If someone needs a better approximation than you’ve already given, they pop the next one off.

Streams give you some inverted control flow. They allow the results to pull on the input, going against the grain of the ordinary direction of computation. If you are interested in a final result of a certain accuracy, they seem somewhat inefficient. You have to search for the right amount to pull the incoming streams, and the intermediate computations may not be helpful.

Haskell chews infinite lists up for breakfast, so it’s a convenient place for such things https://wiki.haskell.org/Exact_real_arithmetic https://hackage.haskell.org/package/exact-real

A related but slightly different set of methods comes in the form of interval arithmetic. Interval arithmetic also gives precise statements of accuracy, maintain bounds of the accuracy as a number is carried along

Interval arithmetic is very much like forward mode differentiation. In forward mode differentiation, you compute on dual numbers (x,dx) and carry along the derivatives as you go.

type ForwardMode x dx y dy = (x,dx) -> (y,dy)
type IntervalFun x delx y dely = (x,delx) -> (y, dely)

Conceptually, differentiation and these validated bounds are connected as well. They are both telling you something about how the function is behaving nearby. The derivative is mostly meaningful at exactly the point it is evaluated. It is extremely local. The verified bounds being carried along are sort of a very principled finite difference approximation.

But reverse mode differentiation is often where it is at. This is the algorithm that drives deep learning. Reverse mode differentiation can be modeled functionally as a kind of lens. http://www.philipzucker.com/reverse-mode-differentiation-is-kind-of-like-a-lens-ii/ . The thing that makes reverse mode confusing is the backward pass. This is also inverted control flow, where the output pushes information to the input. The Lens structure does this too

type Lens s t a b = s -> (a, b -> t)

It carrier a function that goes in the reverse direction which are being composed in the opposite direction of ordinary control flow. These functions are the “setters” in the ordinary usage of the Lens, but they are the backproppers for differentiation.

By analogy one might try

type RealF x delta y epsilon = Lens x delta y epsilon = x -> (y, epsilon -> delta)

There is something pleasing here compared to interval arithmetic in that the output epsilon drives the input delta. The second function is kind of a Skolemized $\delta(\epsilon)$ from the definition of continuity.

Although it kind of makes sense, there is something unsatisfying about this. How do you compute the x -> y? You already need to know the accuracy before you can make this function?

So it seems to me that actually a better definition is

type RealF x delta y epsilon = Lens epsilon y delta x  = epsilon -> (delta, x -> y)

This type surprised me and is rather nice in many respects. It let’s you actually calculate x -> y, has that lazy pull based feel without infinite streams, and has delta as a function of epsilon.

I have heard, although don’t understand, that uniform continuity is the more constructive definition (see constructive analysis by Bridger) https://en.wikipedia.org/wiki/Uniform_continuity This definition seems to match that.

In addition we are able to use approximations of the actual function if we know the accuracy it needs to be computed to. For example, given we know we need 0.01 accuracy of the output, we know we only need 0.009 accuracy in the input and we only need the x term of a Taylor series of sine (the total inaccuracy of the input and the inaccuracy of our approximation of sine combine to give total inaccuracy of output). If we know the needed accuracy allows it, we can work with fast floating point operations. If we need better we can switch over to mpfr, etc.

This seems nice for MetaOcaml staging or other compile time macro techniques. If the epsilon required is known at compile time, it makes sense to me that one could use MetaOcaml to produce fast unrolled code. In addition, if you know the needed accuracy you can switch between methods and avoid the runtime overhead. The stream based approach seems to have a lot of context switching and perhaps unnecessary intermediate computations. It isn’t as bad as it seems, since these intermediate computations are usually necessary to compute anyhow, but still.

We can play the same monoidal category games with these lenses as ever. We can use dup, par, add, mul, sin, cos etc. and wire things up in diagrams and what have you.

This might be a nice type for use in a theorem prover. The Lens type combined with the appropriate properties that the intervals go to zero and stay consistent for arbitrary epsilon seems like enough? { Realf | something something something}

Relation to Backwards error analysis?

Does this have nice properties like backprop when on high dimensional inputs? That’s where backprop really shines, high to low dimensional functions

## Categorical Combinators for Convex Optimization and Model Predictive Control using Cvxpy

We’re gonna pump this well until someone MAKES me stop.

This particular example is something that I’ve been trying to figure out for a long time, and I am pleasantly surprised at how simple it all seems to be. The key difference with my previous abortive attempts is that I’m not attempting the heavy computational lifting myself.

We can take pointful DSLs and convert them into point-free category theory inspired interface. In this case a very excellent pointful dsl for convex optimization: cvxpy. Some similar and related posts converting dsls to categorical form

A convex optimization problem optimizes a convex objective function with constraints that define a convex set like polytopes or balls. They are polynomial time tractable and shockingly useful. We can make a category out of convex optimization problems. We consider some variables to be “input” and some to be “output”. This choice is somewhat arbitrary as is the case for many “relation” feeling things that aren’t really so rigidly oriented.

Convex programming problems do have a natural notion of composition. Check out the last chapter of Rockafeller, where he talks about the convex algebra of bifunctions. Instead of summing over the inner composition variable like in Vect $\sum_j A_{ij}B_{jk}$, or existentializing like in Rel $\{ (a,c) |\exists b. (a,b)\in A, (b,c) \in B \}$, we instead minimize over the inner composition variable $min_y A(x,y) + B(y,z)$. These are similar operations in that they all produce bound variables.

The identity morphism is just the simple constraint that the input variables equal to output variables with an objective function of 0. This is an affine constraint, hence convex.

In general, if we ignore the objective part entirely by just setting it to zero, we’re actually working in a very computationally useful subcategory of Rel, ConvexRel, the category of relations which are convex sets. Composition corresponds to an existential operation, which is quickly solvable by convex optimization techniques. In operations research terms, these are feasibility problems rather than optimization problems. Many of the combinators do nothing to the objective.

The monoidal product just stacks variables side by side and adds the objectives and combines the constraints. They really are still independent problems. Writing things in this way opens up a possibility for parallelism. More on that some other day.

We can code this all up in python with little combinators that return the input, output, objective, constraintlist. We need to hide these in inner lambdas for appropriate fresh generation of variables.

Now for a somewhat more concrete example: Model Predictive control of an unstable (linearized) pendulum.

Model predictive control is where you solve an optimization problem of the finite time rollout of a control system online. In other words, you take measurement of the current state, update the constraint in an optimization problem, ask the solver to solve it, and then apply the force or controls that the solver says is the best.

This gives the advantage over the LQR controller in that you can set hard inequality bounds on total force available, or positions where you wish to allow the thing to go. You don’t want your system crashing into some wall or falling over some cliff for example. These really are useful constraints in practice. You can also include possibly time dependent aspects of the dynamics of your system, possibly helping you model nonlinear dynamics of your system.

Here we model the unstable point of a pendulum and ask the controller to find forces to balance the pendulum.

We can interpret the controller in GraphCat in order to produce a diagram of the 10 step lookahead controller. This is an advantage of the categorical style a la compiling to categories

We can also actually run it in model predictive control configuration in simulation.

### Bits and Bobbles

ADMM – It’s a “lens”. I’m pretty sure I know how to do it pointfree. Let’s do it next time.

The minimization can be bubbled out to the top is we are always minimizing. If we mix in maximization, then we can’t and we’re working on a more difficult problem. This is similar to what happens in Rel when you have relational division, which is a kind of universal quantification $\forall$ . Mixed quantifier problems in general are very tough. These kinds of problems include games, synthesis, and robustness. More on this some other day.

Convex-Concave programming minimax https://web.stanford.edu/~boyd/papers/pdf/dccp_cdc.pdf https://web.stanford.edu/class/ee364b/lectures/cvxccv.pdf

The minimization operation can be related to the summation operation by the method of steepest descent in some cases. The method of steepest descent approximates a sum or integral by evaluating it at it’s most dominant position and expanding out from there, hence converts a linear algebra thing into an optimization problem. Examples include the connection between statistical mechanics and thermodynamics and classical mechanics and quantum mechanics.

Legendre Transformation ~ Laplace Transformation via steepest descent https://en.wikipedia.org/wiki/Convex_conjugate yada yada, all kinds of good stuff.

Intersection is easy. Join/union is harder. Does MIP help?

def meet(f,g):
def res():
x,y,o,c = f()
x1,y1,o1,c1 = g()
return x,y,o+o1, c+ c1 + [x ==  x1, y == y1]
return res

Quantifier elimination

## Rough Ideas on Categorical Combinators for Model Checking Petri Nets using Cvxpy

Petri nets are a framework for modeling dynamical systems that is very intuitive to some people. The vanilla version is that there are discrete tokens at nodes on a graph representing resources of some kind and tokens can be combined according to the firing of transition rules into new tokens in some other location.

This is a natural generalization of chemical reaction kinetics, where tokens are particular kinds of atoms that need to come together. It also is a useful notion for computer systems, where tokens represent some computational resource.

To me, this becomes rather similar to a flow problem or circuit problem. Tokens feel a bit like charge transitions are a bit like current (although not necessarily conservative). In a circuit, one can have such a small current that the particulate nature of electric current in terms of electrons is important. This happens for shot noise or for coulomb blockade for example.

If the number of tokens is very large, it seems intuitively sensible to me that one can well approximate the behavior by relaxing to a continuum. Circuits have discrete electrons and yet are very well approximated by ohm’s laws and the like. Populations are made of individuals, and yet in the thousands their dynamics are well described by differential equations.

It seems to me that mixed integer programming is a natural fit for this problem. Mixed integer programming has had its implementations and theory heavily refined for over 70 years so now very general purpose and performant off the shelf solvers are available. The way mixed integer programs are solved is by considering their quickly solved continuous relaxation (allowing fractional tokens and fractional transitions more akin to continuous electrical circuit flow) and using this information to systematically inform a discrete search process. This seems to me a reasonable starting approximation. Another name for petri nets is Vector Addition Systems, which has more of the matrix-y flavor.

We can encode a bounded model checking for reachability of a petri net into a mixed integer program fairly easily. We use 2-index variables, the first of which will be used for time step. We again turn to the general purpose functional way of encoding pointful dsls into pointfree ones as I have done here and here. The key point is that you need to be careful where you generate fresh variables. This is basically copy catting my posts here. http://www.philipzucker.com/categorical-combinators-for-graphviz-in-python/ http://www.philipzucker.com/a-sketch-of-categorical-relation-algebra-combinators-in-z3py/

I’m like 70% sure what I did here makes sense, but I’m pretty sure the general idea makes sense with some fiddling.

The big piece is the weighted_block function. It let’s you build a combinator with an internal state and input and output flow variables. You give matrices with entries for every possible transition. Whether transitions occurred between $t$ and $t+1$ is indicated by integer variables. There is also possible accumulation of tokens at nodes, which also requires integer variables. Perhaps we’d want to expose the token state of the nodes to the outside too?

We can also get out a graphical representation of the net by reinterpreting our program into GraphCat. This is part of the power of the categorical interface. http://www.philipzucker.com/categorical-combinators-for-graphviz-in-python/

When I talked to Zach about this, he seemed skeptical that MIP solvers wouldn’t eat die a horrible death if you threw a moderately large petri net into them. Hard to say without trying.

#### Thoughts

There is an interesting analogy to be found with quantum field theory in that if you lift up to considering distributions of tokens, it looks like an occupation number representation. See Baez. http://math.ucr.edu/home/baez/stoch_stable.pdf

If you relax the integer constraint and the positivity constraints, this really is a finite difference formulation for capacitor circuits. The internal states would then be the charge of the capacitor. Would the positivity constraint be useful for diodes?

I wonder how relevant the chunky nature of petri nets might be for considering superconducting circuits, which have quantization of quantities from quantum mechanical effects.

Cvxpy let’s you describe convex regions. We can use this to implement a the convex subcategory of Rel which you can ask reachability questions. Relational division won’t work probably. I wonder if there is something fun there with respect the the integerizing operation and galois connections.

Edit: I should have googled a bit first. https://www.sciencedirect.com/science/article/pii/S0377221705009240 mathemtical programming tecchniques for petri net reachability. So it has been tried, and it sounds like the results weren’t insanely bad.

## Categorical Combinators for Graphviz in Python

Graphviz is a graph visualization tool https://www.graphviz.org/. In Conal Elliott’s Compiling to categories http://conal.net/papers/compiling-to-categories/, compiling code to its corresponding graphviz representation was one very compelling example. These graphs are very similar to the corresponding string diagram of the monoidal category expression, but they also look like boolean circuit diagrams. Besides in Conal Elliott’s Haskell implementation, there is an implementation in the Julia Catlab.jl project https://epatters.github.io/Catlab.jl/stable/

I’ve basically implemented a toy version of a similar thing in python. It lets you do things like this

Why python?

• Python is the lingua franca of computing these days. Many people encounter it, even people whose main thing isn’t computers.
• The python ecosystem is nutso good.
• Julia is kind of an uphill battle for me. I’m fighting the battle ( https://github.com/philzook58/Rel.jl ) , but I already know python pretty well. I can rip this out and move on.

What I did was implement some wrappers around the graphviz python package. It exposes a not very feature rich stateful interface. It is pretty nice that it prints the graphs inline in jupyter notebooks though.

The code is written in a style very similar (and hopefully overloadable with) to that of z3py relation algebra. http://www.philipzucker.com/a-sketch-of-categorical-relation-algebra-combinators-in-z3py/ . There is a fairly general cookbook method here for categorifying dsl. Since graphviz does not directly expose fresh node creation as far as I can tell, I made my own using a random number generator. The actual combinators are graphviz object processors, so we build up a giant functional chain of processors and then actually execute it with run. The inputs and outputs are represented by lists of node names. The is some design space to consider here.

I also had to use class based wrappers Based on the precedent set by the python 3 matrix multiplication operator @, I think it is a requirement that this also be used for category composition. id is a keyword or something in python unfortunately. For monoidal product, I feel like overloading power ** looks nice even if it is a nonsensical analogy, * is also not too bad. I went with * for now.

The graphviz graphs aren’t quite string diagrams. They make no promise to preserve the ordering of your operations, but they seem to tend to.

Here’s some example usage

cup = GraphCat.cup()
cap = GraphCat.cap()
d =  cap @ (I * I) @ cup  #(I * cap) @ (I * I * I) @ (cup * I)
d.run()
d = plus @ (GC.const(1) * GC.const(2))
d = d.run()

GC = GraphCat
f = GraphCat.named_simple("f")
g = GraphCat.named_simple("g")
I = GraphCat.idd()
dump = GC.dump()
dup = GC.dup()
diagram = ((f * I) @ dup @ g @ (dump * I)  @ (I * f) @ (f * f)) * g
diagram.run()

# by passing in different category classes, we can make polymorphic functions
# They have to have a uniform interface though, which is hard to constrain in python.
def polymorphic_prog(M):
idd = M.idd()
dump = M.dump()
dup = M.dup()
return (idd * dump) @ dup
polymorphic_prog(GraphCat).run()

For example something like this ought to work. Then you can get the graph of some matrix computation to go along with it’s numpy implementation

class FinVect(np.ndarray):

def compose(f,g):
return f @ g
def idd(n):
return np.eye(n)
def par(f,g):
return np.kron(f,g)
def __mult__(self,rhs):
return np.kron(f,g)
# and so on. 

Maybe outputting tikz is promising? https://github.com/negrinho/sane_tikz

## A Sketch of Categorical Relation Algebra Combinators in Z3Py

I’ve discussed relation algebra before. Relations are sets of tuples. There, I implemented the relations naively using lists for sets. This is very simple, and very clean especially with list comprehension syntax. It is however horrifically inefficient, and we could only deal with finitely enumerable domains. The easiest path to fixing these problems is to cash out to an external solver, in this case z3.

There are many beautifully implemented solvers out there and equally beautiful DSL/modeling languages. Examples in mind include sympy, cvxpy, and z3. These modeling languages require you to instantiate variable objects and build expressions out of them and then hand it off to the solver. This is a reasonable interface, but there are advantages to a more categorical/point-free style DSL.

Point-free languages are ones that do not include binding forms that introduce bound/dummy variables. Examples of binding forms like this are $\lambda \sum \max \min \int \sup \lim \forall \exists$. One problem lies in the fact that the names of bound variables don’t matter, and that they end up accidentally smashing into each other. You may have experienced this in physics or math class as the dummy indices or dummy variable problem causing you to screw up your calculation of some cross product identity or some complicated tensor sum. These are surprisingly subtle problems, very difficult to diagnose and get right. de Bruijn indices is a technique for giving the bound variables canonical names, but it sucks to implement in its own way. When you make a DSL point free, it is a joy to manipulate, optimize, and search. I think this may be the core of why category theory is good language for mathematics and programming.

Point-free style also tends to have significant economy of size, for better or worse. Sometimes it is better to have an expression very dense in information. This is important if you are about the algebraically manipulate an expression with paper and pencil. Every manipulation requires a great deal of mind numbing copying as you proceed line by line, so it can be excruciating if your notation has a lot of unnecessary bulk.

Relations are like functions. The two pieces of the tuple can be roughly thought of as the “input” and the “output”. Relations are only loosely directional though. Part of the point of relations is that the converse (inverse) of a relation is easy to define.

When we are implement relations, we have a choice. Do we want the relation to produce its variables, accept its variable, or accept one and produce the other? There are advantages to each. When relations were [(a,b)], a -> b -> Bool, and a -> [b] converting between these forms was a rather painful enumeration process. The sting of converting between them is taken out by the fact that the conversion is no longer a very computationally expensive process, since we’re working at the modeling layer.

When you’re converting a pointful DSL to pointfree DSL, you have to be careful where you instantiate fresh variables or else you’ll end up with secret relations that you didn’t intend. Every instantiation of id needs to be using fresh variables for example. You don’t want the different id talking to each other. Sometimes achieving this involves a little currying and/or thunking.

There is a pattern that I have notice when I’m using modeling languages. When you have a function or relation on variables, there are constraints produced that you have to keep a record of. The pythonic way is to have a Model or Solver object, and then have that objects mutate an internal record of the set of constraints. I don’t particularly enjoy this style though. It feels like too much boiler plate.

In Haskell, I would use something like a Writer monad to automatically record the constraints that are occurring. Monads are not really all that pleasant even in Haskell, and especially a no go in python without “do” syntax.

However, because we are going point free it is no extra cost at all to include this pipework along for the ride in the composition operation.

Here are implementations of the identity and composition for three different styles. Style 1 is fully receptive, style 2 is mixed (function feeling) and style 3 is fully productive of variables.

Fair warning, I’m being sketchy here. I haven’t really tried this stuff out.

z3 is a simply typed language. You can get away with some polymorphism at the python level (for example the == dispatches correctly accord to the object) but sometimes you need to manually specify the sort of the variables. Given these types, the different styles are interconvertible

We can create the general cadre of relation algebra operators. Here is a somewhat incomplete list

Questions about relation algebra expressions are often phrased in term of relational inclusion. You can construct a relation algebra expression, use the rsub in the appropriate way and ask z3’s prove function if it is true.

Z3 has solvers for

• Combinatorial Relations
• Linear Relations
• Polyhedral Relations
• Polynomial Relations
• Interval Relations – A point I was confused on. I thought interval relations were not interesting. But I was interpetting the term incorrectly. I was thinking of relations on AxB that are constrained to take the form of a product of intervals. In this case, the choice of A has no effect on the possible B whatsoever, so it feels non relational. However, there is also I_A x I_B , relations over the intervals of A and B. This is much closer to what is actually being discussed in interval arithmetic.

Applications we can use this for:

• Graph Problems. The Edges can be thought of as a relation between vertices. Relation composition Using the starn operator is a way to ask for paths through the graph.
• Linear Relations – To some degree this might supplant my efforts on linear relations. http://www.philipzucker.com/linear-relation-algebra-of-circuits-with-hmatrix/ Z3 is fully capable of understanding linear relations.
• Safety and liveness of control systems. Again. a transition relation is natural here. It is conceivable that the state space can be heterogenous in time, which is the interesting power of the categorical style. I feel like traditional control systems usually maintain the same state space throughout.
• Program verification
• Games? Nash equilibria?

### Other Thoughts

• Maybe we are just building a shitty version of alloy. https://alloytools.org/
• What about uninterpeted relations? What about higher order relations? What about reflecting into a z3 ADT for a relational language. Then we could do relational program synthesis. This is one style, just hand everything off to smt. https://github.com/nadia-polikarpova/cse291-program-synthesis/tree/master/lectures
• I should try to comply with python conventions, in particular numpy and pandas conventions. @ should be composition for example, since relation composition has a lot of flavor of matrix composition. I should overload a lot of operators, but then I’d need to wrap in a class 🙁
• Z3 has special support for some relations. How does that play in? https://theory.stanford.edu/~nikolaj/programmingz3.html#sec-special-relations https://z3prover.github.io/api/html/ml/Z3.Relation.html
• As long as you only use composition, there is a chaining of existentials, which really isn’t so bad.
• What we’ve done here is basically analogous/identical to what John Wiegley did compiling to the category of z3. Slightly different in that he only allowed for existential composition rather than relational division. http://newartisans.com/2017/04/haskell-and-z3/
• We can reduced the burden on z3 if we know the constructive proof objects that witness our various operations. Z3 is gonna do better if we can tell it exactly which y witness the composition of operators, or clues to which branch of an Or it should use.
• It’s a bummer, but when you use quantifiers, you don’t see countermodels? Maybe there is some hook where you can, or in the dump of the proof object.
• What about recursion schemes? The exact nature of z3 to handle unbounded problems is fuzzy to me. It does have the support to define recursive functions. Also explicit induction predicates can go through sometimes. Maybe look at the Cata I made in fancy relaion algebra post
• I think most proof assistants have implementations of relation algebra available. I find you can do a surprising amount in z3.

## Solving the Laplace Equations with Linear Relations

The Laplace equation is ubiquitous in physics and engineering.

\$latex \nabla^2 \phi = 0 = \partial_x^2 \phi + \partial_y^2 \phi = 0

It and slight variants of it describes electrostatics, magnetostatics, steady state heat flow, elastic flex, pressure, velocity potentials.

There are a couple reasons for that.

• It results from minimizing the squared gradient of a field $|\nabla \phi |^2$ which can make sense from an energy minimization perspective.
• Similarly it results from the combination of a flow conservation law and a linear constitutive relation connecting flow and field (such as Ohm’s law, Fick’s law, or Hooke’s law).
• It also gets used even if not particularly appropriate because we know how to mathematically deal with it, for example in image processing.

There are a couple of questions we may want to ask about a Laplace equation system

• Given the field on the boundary, determine the field in the interior (Dirchlet problem)
• Given the normal derivative of the field on the boundary determine the field in the interior (Neumann problem)
• Given sources in the interior and 0 boundary condition, determine the field. The Laplace equation is called the Poisson equation when you allow a source term on the right hand side. $\nabla^2 \phi = \rho$.
• Given the field at the boundary, determine the derivative at the boundary. Dirichlet-to-Neumann map or Poincare-Steklov operator.

Given the Dirichlet to Neumann map, you do not have to consider the interior of a region to use it. The Dirichlet to Neumann map is sort of the same thing as an effective resistance or scattering matrix. It gives you a black box representation of a region based solely on the variables at its boundary.

This linear relation algebra is useful for many things that I’d have considered a use case for the Schur complement. The Schur complement arises when you do Gaussian elimination on a blocked matrix. It is good that this pattern has a name, because once you know about it, you’ll see it in many places. Domain decomposition, marginalized gaussian distributions, low-rank update, Scattering matrices.

By composing the linear relations corresponding to the Dirchlet-Neumann relations of regions, we can build the Dirichlet-Neumann relations of larger regions.

To make this more concrete, let us take the example of electrical circuits like before. A grid of resistors is a finite difference approximation to the continuous problem

$-\nabla \phi = E$ Electric field is gradient of potential

$E = \rho j$ continuum ohm’s law

$\nabla\cdot j = 0$ current conservation

In this post, I mentioned how you can make reasonable 2 dimensional diagrams out of a monoidal category, by sort of arbitrarily flipping one wire up and one wire down as in the diagram below. This defines a horizontal and vertical composition which have to do the required book-keeping (associations) to keep an arrow in canonical form. I had considered this for the management method of weights in neural networks, but it is way more natural as the actual geometrical layout of a finite difference grid of a laplace equation.

So we can reuse our categorical circuit combinators to build a finite difference Laplace equation.

This can be implemented in Haskell doing the following. Neato.

### Bits and Bobbles

• Not the tightest post, but I needed to get it out there. I have a short attention span.
• Homology and defining simplices as categories. One way of describing Homology is about linear operators that are analogues of finite difference operators (or better yet, discrete differential geometry operators / exterior derivatives). To some degree, it is analyzing the required boundary conditions to fully define differential equations on weirdo topological surfaces, which correspond to geometrical loops/holes. You can figure this out by looking at subspaces and quotients of the difference operators. Here we have here a very category theory way of looking at partial differential equations. How does it all connect?
• Continuous circuit models – https://en.wikipedia.org/wiki/Distributed-element_model Telegrapher’s equation is classic example.
• Cody mentioned that I could actually build circuits and measure categorical identities in a sense. That’s kind of cool. Or I could draw conductive ink on carbon paper and actually make my string diagrams into circuits? That is also brain tickling
• Network circuits
• I really want to get coefficients that aren’t just doubles. allowing rational functions of a frequency $\omega$ would allow analysis of capacitor/inductor circuits, but also tight binding model systems for fun things like topological insulators and the Haldane model http://www.philipzucker.com/topologically-non-trivial-circuit-making-haldane-model-gyrator/ . I may need to leave Haskell. I’m not seeing quite the functionality I need. Use Sympy? https://arxiv.org/abs/1605.02532 HLinear. Flint bindings for haskell? Looks unmaintained. Could also use a grobner basis package as dynamite for a mouse.
• This is relevant for the boundary element method. Some really cool other stuff relevant here. http://people.maths.ox.ac.uk/martinsson/2014_CBMS/

Blah Blah blah: The subtlest aspect of differential equations is that of boundary conditions. It is more correct usually to consider the system of the interior differential equation and the boundary conditions as equally essential parts of the statement of the problem you are considering.

## Categorical LQR Control with Linear Relations

Last time, I described and built an interesting expansion of describing systems via linear functions, that of using linear relations. We remove the requirement that mappings be functional (exactly one output vector for any given input vector), which extends our descriptive capability. This is useful for describing “open” pieces of a linear system like electric circuits. This blog post is about another application: linear dynamical systems and control.

Linear relations are an excellent tool for reachability/controllability. In a control system, it is important to know where it is possible to get the system to. With linear dynamics $x_{t+1} = Ax_{t} + B u_{t}$, an easy controllability question is “can my system reach into some subspace”. This isn’t quite the most natural question physically, but it is natural mathematically. My first impulse would be to ask “given the state starts in this little region over here, can it get to this little region over here”, but the subspace question is a bit easier to answer. It’s a little funky but it isn’t useless. It can detect if the control parameter only touches 1 of 2 independent dynamical systems for example. We can write the equations of motion as a linear relation and iterate composition on them. See Erbele for more.

There is a set of different things (and kind of more interesting things) that are under the purview of linear control theory, LQR Controllers and Kalman filters. The LQR controller and Kalman filter are roughly (exactly?) the same thing mathematically. At an abstract mathematical level, they both rely on the fact that optimization of a quadratic objective $x^T Q x + r^T x + c$ with a linear constraints $Ax=b$ is solvable in closed form via linear algebra. The cost of the LQR controller could be the squared distance to some goal position for example. When you optimize a function, you set the derivative to 0. This is a linear equation for quadratic objectives. It is a useful framework because it has such powerful computational teeth.

The Kalman filter does a similar thing, except for the problem of state estimation. There are measurements linear related to the state that you want to match with the prior knowledge of the linear dynamics of the system and expected errors of measurement and environment perturbations to the dynamics.

There are a couple different related species of these filters. We could consider discrete time or continuous time. We can also consider infinite horizon or finite horizon. I feel that discrete time and finite horizon are the most simple and fundamental so that is what we’ll stick with. The infinite horizon and continuous time are limiting cases.

We also can consider the dynamics to be fixed for all time steps, or varying with time. Varying with time is useful for the approximation of nonlinear systems, where there are different good nonlinear approximation (taylor series of the dynamics) depending on the current state.

There are a couple ways to solve a constrained quadratic optimization problem. In some sense, the most conceptually straightforward is just to solve for a span of the basis (the “V-Rep” of my previous post) and plug that in to the quadratic objective and optimize over your now unconstrained problem. However, it is commonplace and elegant in many respects to use the Lagrange multiplier method. You introduce a new parameter for every linear equality and add a term to the objective $\lambda^T (A x - b)$. Hypothetically this term is 0 for the constrained solution so we haven’t changed the objective in a sense. It’s a funny slight of hand. If you optimize over x and $\lambda$, the equality constraint comes out as your gradient conditions on $\lambda$. Via this method, we convert a linearly constrained quadratic optimization problem into an unconstrained quadratic optimization problem with more variables.

Despite feeling very abstract, the value these Lagrangian variables take on has an interpretation. They are the “cost” or “price” of the equality they correspond to. If you moved the constraint by an amount $Ax - b + \epsilon$, you would change the optimal cost by an amount $\lambda \epsilon$. (Pretty sure I have that right. Units check out. See Boyd https://www.youtube.com/watch?v=FJVmflArCXc)

The Lagrange multipliers enforcing the linear dynamics are called the co-state variables. They represent the “price” that the dynamics cost, and are derivatives of the optimal value function V(s) (The best value that can be achieved from state s) that may be familiar to you from dynamic programming or reinforcement learning. See references below for more.

Let’s get down to some brass tacks. I’ve suppressed some terms for simplicity. You can also add offsets to the dynamics and costs.

A quadratic cost function with lagrange multipliers. Q is a cost matrix associated with the x state variables, R is a cost matrix for the u control variables.

$C = \lambda_0 (x_0 - \tilde{x}_0) + \sum_t x_t^T Q x_t + u_t^T R u_t + \lambda_{t+1}^T (x_{t+1} - A x_t - B u_t )$

Equations of motion results from optimizing with respect to $\lambda$ by design.

$\nabla_{\lambda_{t+1}} C = x_{t+1} - A x_t - B u_t = 0$.

The initial conditions are enforced by the zeroth multiplier.

$\nabla_{\lambda_0} C = x_i - x_{0} = 0$

Differentiation with respect to the state x has the interpretation of backwards iteration of value derivative, somewhat related to what one finds in the Bellman equation.

$\nabla_{x_t} C = Q x_{t} + A^T \lambda_{t+1} - \lambda_{t} = 0 \Longrightarrow \lambda_{t} = A^T \lambda_{t+1} + Q x_{t}$

The final condition on value derivative is the one that makes it the most clear that the Lagrange multiplier has the interpretation of the derivative of the value function, as it sets it to that.

$\nabla_{x_N} C = Q x_N - \lambda_{N} = 0$

Finally, differentiation with respect to the control picks the best action given knowledge of the value function at that time step.

$\nabla_{u_t} C = R u_{t} - B^T \lambda_t = 0$

Ok. Let’s code it up using linear relations. Each of these conditions is a separate little conceptual box. We can build the optimal control step relation by combining these updates together

The following is a bit sketchy. I am confident it makes sense, but I’m not confident that I have all of the signs and other details correct. I also still need to add the linear terms to the objective and offset terms to the dynamics. These details are all kind of actually important. Still, I think it’s nice to set down in preliminary blog form.

### Bits and Bobbles

• The code in context https://github.com/philzook58/ConvexCat/blob/master/src/LinRel.hs
• Some of the juicier stuff is nonlinear control. Gotta walk before we can run though. I have some suspicions that a streaming library may be useful here, or a lens-related approach. Also ADMM.
• Reminiscent of Keldysh contour. Probably a meaningless coincidence.
• In some sense H-Rep is the analog of (a -> b -> Bool) and V-rep [(a,b)]
• Note that the equations of motion are relational rather than functional for a control systems. The control parameters $u$ describe undetermined variables under our control.
• Loopback (trace) the value derivative for infinite horizon control.
• Can solve the Laplace equation with a Poincare Steklov operator. That should be my next post.
• There is something a touch unsatisfying even with the reduced goals of this post. Why did I have to write down the quadratic optimization problem and then hand translate it to linear relations? It’s kind of unacceptable. The quadratic optimization problem is really the most natural statement, but I haven’t figured out to make it compositional. The last chapter of Rockafellar?

### References

https://arxiv.org/abs/1405.6881 Baez and Erbele – Categories in Control

http://www.scholarpedia.org/article/Optimal_control

http://www.argmin.net/2016/05/18/mates-of-costate/ – interesting analogy to backpropagation. Lens connection?

https://courses.cs.washington.edu/courses/cse528/09sp/optimality_chapter.pdf