Last time I explained how to create the ‘maximal abelian cover’ of a connected graph. Now I’ll say more about a systematic procedure for embedding this into a vector space. That will give us a topological crystal, like the one above.

Some remarkably symmetrical patterns arise this way! For example, starting from this graph:

we get this:

Nature uses this pattern for crystals of graphene.

Starting from this graph:

we get this:

Nature uses this for crystals of diamond! Since the construction depends only on the topology of the graph we start with, we call this embedded copy of its maximal abelian cover a **topological crystal**.

Today I’ll remind you how this construction works. I’ll also outline a proof that it gives an *embedding* of the maximal abelian cover if and only if the graph has no **bridges**: that is, edges that disconnect the graph when removed. I’ll skip all the hard steps of the proof, but they can be found here:

• John Baez, Topological crystals.

### The homology of graphs

I’ll start with some standard stuff that’s good to know. Let be a graph. Remember from last time that we’re working in a setup where every edge goes from a vertex called its **source** to a vertex called its **target** . We write to indicate that is going from to . You can think of the edge as having an arrow on it, and if you turn the arrow around you get the **inverse** edge, . Also, .

The group of **integral 0-chains** on , , is the free abelian group on the set of vertices of . The group of **integral 1-chains** on , , is the quotient of the free abelian group on the set of edges of by relations for every edge . The **boundary map** is the homomorphism

such that

for each edge , and

is the group of **integral 1-cycles** on .

Remember, a **path** in a graph is a sequence of edges, the target of each one being the source of the next. Any path in determines an integral 1-chain:

For any path we have

and if and are composable then

Last time I explained what it means for two paths to be ‘homologous’. Here’s the quick way to say it. There’s groupoid called the **fundamental groupoid** of , where the objects are the vertices of and the morphisms are freely generated by the edges except for relations saying that the inverse of really is . We can **abelianize** the fundamental groupoid by imposing relations saying that whenever this equation makes sense. Each path gives a morphism which I’ll call in the abelianized fundamental groupoid. We say two paths are **homologous** if .

Here’s a nice thing:

**Lemma A.** Let be a graph. Two paths in are homologous if and only if they give the same 1-chain: .

**Proof.** See the paper. You could say they give ‘homologous’ 1-chains, too, but for graphs that’s the same as being equal. █

We define vector spaces of **0-chains** and **1-chains** by

respectively. We extend the boundary map to a linear map

We let be the kernel of this linear map, or equivalently,

and we call elements of this vector space **1-cycles**. Since is a free abelian group, it forms a lattice in the space of 1-cycles. Any edge of can be seen as a 1-chain, and there is a unique inner product on such that edges form an orthonormal basis (with each edge counting as the negative of .) There is thus an orthogonal projection

This is the key to building topological crystals!

### The embedding of atoms

We now come to the main construction, first introduced by Kotani and Sunada. To build a topological crystal, we start with a connected graph with a chosen basepoint . We define an **atom** to be a homology class of paths starting at the basepoint, like

Last time I showed that these atoms are the vertices of the maximal abelian cover of . Now let’s embed these atoms in a vector space!

**Definition.** Let be a connected graph with a chosen basepoint. Let be its set of atoms. Define the map

by

That is well-defined follows from Lemma A. The interesting part is this:

**Theorem A.** The following are equivalent:

(1) The graph has no bridges.

(2) The map is one-to-one.

**Proof.** The map is one-to-one if and only if for any atoms and , implies . Note that is a path in with , so

Since vanishes if and only if is orthogonal to every 1-cycle, we have

On the other hand, Lemma A says

Thus, to prove (1)(2), it suffices to that show that has no bridges if and only if every 1-chain orthogonal to every 1-cycle has . This is Lemma D below. █

The following lemmas are the key to the theorem above — and also a deeper one saying that if has no bridges, we can extend to an embedding of the whole maximal abelian cover of .

For now, we just need to show that any nonzero 1-chain coming from a path in a bridgeless graph has nonzero inner product with some 1-cycle. The following lemmas, inspired by an idea of Ilya Bogdanov, yield an algorithm for actually constructing such a 1-cycle. This 1-cycle also has other desirable properties, which will come in handy later.

To state these, let a **simple path** be one in which each vertex appears at most once. Let a **simple loop** be a loop in which each vertex except appears at most once, while appears exactly twice, as the starting point and ending point. Let the **support** of a 1-chain , denoted , be the set of edges such that . This excludes edges with , but also those with , which are inverses of edges in the support. Note that

Thus, is the smallest set of edges such that can be written as a positive linear combination of edges in this set.

Okay, here are the lemmas!

**Lemma B.** Let be any graph and let be an integral 1-cycle on . Then for some we can write

where are simple loops with .

**Proof.** See the paper. The proof is an algorithm that builds a simple loop with. We subtract this from , and if the result isn’t zero we repeat the algorithm, continuing to subtract off 1-cycles until there’s nothing left. █

**Lemma C.** Let be a path in a graph . Then for some we can write

where is a simple path and are simple loops with .

**Proof.** This relies on the previous lemma, and the proof is similar — but when we can’t subtract off any more ’s we show what’s left is for a simple path . █

**Lemma D.** Let be a graph. Then the following are equivalent:

(1) has no bridges.

(2) For any path in , if is orthogonal to every 1-cycle then .

**Proof.** It’s easy to show a bridge gives a nonzero 1-chain that’s orthogonal to all 1-cycles, so the hard part is showing that for a bridgeless graph, if is orthogonal to every 1-cycle then . The idea is to start with a path for which . We hit this path with Lemma C, which lets us replace by a simple path . The point is that a simple path is a lot easier to deal with than a general path: a general path could wind around crazily, passing over every edge of our graph multiple times.

Then, assuming has no bridges, we use Ilya Bogdanov’s idea to build a 1-cycle that’s not orthogonal to . The basic idea is to take the path and write it out as . Since the last edge is not a bridge, there must be a path from back to that does not use the edge or its inverse. Combining this path with we can construct a loop, which gives a cycle having nonzero inner product with and thus with .

I’m deliberately glossing over some difficulties that can arise, so see the paper for details! █

### Embedding the whole crystal

Okay: so far, we’ve taken a connected bridgeless graph and embedded its atoms into the space of 1-cycles via a map

These atoms are the vertices of the maximal abelian cover . Now we’ll extend to an embedding of the whole graph — or to be precise, its geometric realization . Remember, for us a graph is an abstract combinatorial gadget; its geometric realization is a topological space where the edges become closed intervals.

The idea is that just as maps each atom to a point in the vector space , maps each edge of to a straight line segment between such points. These line segments serve as the ‘bonds’ of a topological crystal. The only challenge is to show that these bonds do not cross each other.

**Theorem B.** If is a connected graph with basepoint, the map extends to a continuous map

sending each edge of to a straight line segment in . If has no bridges, then is one-to-one.

**Proof.** The first part is easy; the second part takes real work! The problem is to show the edges don’t cross. Greg Egan and I couldn’t do it using just Lemma D above. However, there’s a nice argument that goes back and uses Lemma C — read the paper for details.

As usual, history is different than what you read in math papers: David Speyer gave us a nice proof of Lemma D, and that was good enough to prove that atoms are mapped into the space of 1-cycles in a one-to-one way, but we only came up with Lemma C after weeks of struggling to prove the edges don’t cross. █

### Connections to tropical geometry

Tropical geometry sets up a nice analogy between Riemann surfaces and graphs. The Abel–Jacobi map embeds any Riemann surface in its Jacobian, which is the torus . We can similarly define the Jacobian of a graph to be . Theorem B yields a way to embed a graph, or more precisely its geometric realization , into its Jacobian. This is the analogue, for graphs, of the Abel–Jacobi map.

After I put this paper on the arXiv, I got an email from Matt Baker saying that he had already proved Theorem A — or to be precise, something that’s clearly equivalent. It’s Theorem 1.8 here:

• Matthew Baker and Serguei Norine, Riemann–Roch and Abel–Jacobi theory on a finite graph.

This says that the *vertices* of a bridgeless graph are embedded in its Jacobian by means of the graph-theoretic analogue of the Abel–Jacobi map.

What I really want to know is whether someone’s written up a proof that this map embeds the whole graph, not just its vertices, into its Jacobian in a one-to-one way. That would imply Theorem B. For more on this, try my conversation with David Speyer.

Anyway, there’s a nice connection between topological crystallography and tropical geometry, and not enough communication between the two communities. Once I figure out what the tropical folks have proved, I will revise my paper to take that into account.

Next time I’ll talk about more *examples* of topological crystals!

### Read the whole series

• Part 1 – the basic idea.

• Part 2 – the maximal abelian cover of a graph.

• Part 3 – constructing topological crystals.

• Part 4 – examples of topological crystals.

Dear John. I am excited about the links with tropical geometry. Tropical geometry and non-archimedean mathematics are something I would love to touch at my blog (now paused due to some personal and academical issues). I have enjoyed to see tropical connections with graph theory…

To go beyond: What about tropical spacetime physics or tropical Quantum Mechanics? What about a polycrystalline tropically quantum spacetime?

You can combine ideas in many ways, but throwing them together at random is rarely opimtal. Tropical mathematics is really the ‘classical limit’ or ‘low-temperature limit’ of mathematics using complex numbers. I discussed this in weeks 11, 12 and 13 of my Winter 2007 seminar: you can read the notes. I also recommend this:

• Grigori L. Litvinov, The Maslov dequantization, idempotent and tropical mathematics: a very brief introduction.

I think this is the most promising way to apply tropical mathematics to physics.

OH, I did not remember that! You have been so prolific than I forgot your QG seminar touching this fascinating topic. What about a p-adic/tropical geometry dictionary? Does it exist if any? It is interesting your comment about tropical math as the “classical” limit of quantum math. Low temperature physics is purely quantum at nature (e.g., see the BEC phase transition!). Tropical mathematics is yet a young branch but I am sure physisics will face with it much more in the near future.

Interesting…Tropical mathematics as “low T limit of mathematics”. I will reread your winter 2007 seminar…I had almost forgotten it completely! And what about the high temperature limit?

Good puzzle! You can work it out yourself using the formulas on page 18 here.

While I try to digest the maths, on the version I see there’s two repeated sentences on tbe third-last paragraph.

Thanks! I love it when people catch my typos.

Next time I’ll give tons of examples. All this was just to define the construction and prove it gives a “crystal” embedded in a vector space.

Hey, I’d like to go into medicine myself but I was wondering what made you pick maths and physics. Out of interest 😊. It’s just your passion really comes across.

When I was young, I really wanted to understand

everythingabout the universe—and especially the most basic, fundamental things. So, I wanted to start by learning the laws of physics, since these govern everything. As I went further, I realized that the laws of physics are written in the language of mathematics, so I got interested in that.I also discovered that profound questions like “what is true?” and “how do we know anything?” led people to develop logic. Thanks to a book my dad checked out of the public library, I learned that in the 20th century Gödel and others proved theorems in logic that put limits on what we can prove. So I got interested in logic, which nowadays is another branch of mathematics.

Nowadays I feel I know enough math and physics to start thinking about other things, like global warming, biology, and a general theory of networks. But occasionally I want to work on pure math, so I do projects like this one on topological crystals.

That’s such a great development. Cool.