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Roots of unity and the Big Picture

Published January 14, 2018 by lievenlb

All lattices in the moonshine picture are number-like, that is of the form $M \frac{g}{h}$ with $M$ a positive integer and $0 \leq g < h$ with $(g,h)=1$ . To understand the action of the Bost-Connes algebra on the Big Picture it is sometimes better to view the lattice $M \frac{g}{h}$ as a primitive $h$ -th root of unity, centered at $hM$ .

The distance from $M$ to any of the lattices $M \frac{g}{h}$ is equal to $2 log(h)$ , and the distances from $M$ and $M \frac{g}{h}$ to $hM$ are all equal to $log(h)$ .

For a prime value $h$ , these $h$ lattices are among the $h+1$ lattices branching off at $hM$ in the $h$ -adic tree (the remaining one being $h^2M$ ).

For general $h$ the situation is more complex. Here’s the picture for $h=6$ with edges in the $2$ -adic tree painted blue, those in the $3$ -adic tree red.

$\xymatrix{& & M \frac{1}{2} \ar@[blue]@{-}[d] & \\ & M \ar@[blue]@{-}[r] \ar@[red]@{-}[d] & 2M \ar@[red]@{-}[d] & M \frac{1}{6} \ar@[red]@{-}[d] \\ M \frac{1}{3} \ar@[red]@{-}[r] & 3M \ar@[blue]@{-}[r] \ar@[red]@{-}[d] & \boxed{6 M} \ar@[blue]@{-}[r] & 3M \frac{1}{2} \ar@[red]@{-}[d] \\ & M \frac{2}{3} & & M \frac{5}{6}}$

To describe the moonshine group $(n|h)+e,f,\dots$ (an example was worked out in the tetrahedral snake post), we need to study the action of base-change with the matrix
$x = \begin{bmatrix} 1 & \frac{1}{h} \\ 0 & 1 \end{bmatrix}$
which sends a lattice of the form $M \frac{g}{h}$ with $0 \leq g < h$ to $M \frac{g+M}{h}$ , so is a rotation over $\frac{2 \pi M}{h}$ around $h M$ . But, we also have to describe the base-change action with the matrix $y = \begin{bmatrix} 1 & 0 \\ n & 1 \end{bmatrix}$ and for this we better use the second description of the lattice as $M \frac{g}{h}=(\frac{g'}{h},\frac{1}{h^2M})$ with $g'$ the multiplicative inverse of $g$ modulo $h$ . Under the action by $y$ , the second factor $\frac{1}{h^2M}$ will be fixed, so this time we have to look at all lattices of the form $(\frac{g}{h},\frac{1}{h^2M})$ with $0 \leq g < h$ , which again can be considered as another set of $h$ -th roots of unity, centered at $hM$ . Here's this second interpretation for $h=6$ : $\xymatrix{M \frac{5}{6} \ar@[red]@{-}[d] & & 4M \frac{1}{3} \ar@[red]@{-}[d] & \\ 3M \frac{1}{2} \ar@[blue]@{-}[r] \ar@[red]@{-}[d] & \boxed{6M} \ar@[blue]@{-}[r] \ar@[red]@{-}[d] & 12 M \ar@[red]@{-}[r] \ar@[red]@{-}[d] & 4 M \frac{2}{3} \\ M \frac{1}{6} & 18 M \ar@[blue]@{-}[r] \ar@[blue]@{-}[d] & 36 M & \\ & 9M \frac{1}{2} & & }$ Under $x$ the first set of $h$ -th roots of unity centered at $hM$ is permuted, whereas $y$ permutes the second set of $h$ -th roots of unity.
These interpretations can be used to spot errors in computing the finite groups $\Gamma_0(n|h)/\Gamma_0(n.h)$ .

Here’s part of the calculation of the action of $y$ on the $(360|1)$ -snake (which consists of $60$ -lattices).

First I got a group of order roughly $600.000$ . After correcting some erroneous cycles, the order went down to 6912.

Finally I spotted that I mis-numbered two lattices in the description of $x$ and $y$ , and the order went down to $48$ as it should, because I knew it had to be equal to $C_2 \times C_2 \times A_4$ .

nc-geometry and moonshine?

Published January 12, 2018 by lievenlb

A well-known link between Conway’s Big Picture and non-commutative geometry is given by the Bost-Connes system.

This quantum statistical mechanical system encodes the arithmetic properties of cyclotomic extensions of $\mathbb{Q}$ .

The corresponding Bost-Connes algebra encodes the action by the power-maps on the roots of unity.

It has generators $e_n$ and $e_n^*$ for every natural number $n$ and additional generators $e(\frac{g}{h})$ for every element in the additive group $\mathbb{Q}/\mathbb{Z}$ (which is of course isomorphic to the multiplicative group of roots of unity).

The defining equations are
$\begin{cases} e_n.e(\frac{g}{h}).e_n^* = \rho_n(e(\frac{g}{h})) \\ e_n^*.e(\frac{g}{h}) = \Psi^n(e(\frac{g}{h}).e_n^* \\ e(\frac{g}{h}).e_n = e_n.\Psi^n(e(\frac{g}{h})) \\ e_n.e_m=e_{nm} \\ e_n^*.e_m^* = e_{nm}^* \\ e_n.e_m^* = e_m^*.e_n~\quad~\text{if $(m,n)=1$} \end{cases}$

Here $\Psi^n$ are the power-maps, that is $\Psi^n(e(\frac{g}{h})) = e(\frac{ng}{h}~mod~1)$ , and the maps $\rho_n$ are given by
$\rho_n(e(\frac{g}{h})) = \sum e(\frac{i}{j})$
where the sum is taken over all $\frac{i}{j} \in \mathbb{Q}/\mathbb{Z}$ such that $n.\frac{i}{j}=\frac{g}{h}$ .

Conway’s Big Picture has as its vertices the (equivalence classes of) lattices $M,\frac{g}{h}$ with $M \in \mathbb{Q}_+$ and $\frac{g}{h} \in \mathbb{Q}/\mathbb{Z}$ .

The Bost-Connes algebra acts on the vector-space with basis the vertices of the Big Picture. The action is given by:
$\begin{cases} e_n \ast \frac{c}{d},\frac{g}{h} = \frac{nc}{d},\rho^m(\frac{g}{h})~\quad~\text{with $m=(n,d)$} \\ e_n^* \ast \frac{c}{d},\frac{g}{h} = (n,c) \times \frac{c}{nd},\Psi^{\frac{n}{m}}(\frac{g}{h})~\quad~\text{with $m=(n,c)$} \\ e(\frac{a}{b}) \ast \frac{c}{d},\frac{g}{h} = \frac{c}{d},\Psi^c(\frac{a}{b}) \frac{g}{h} \end{cases}$

This connection makes one wonder whether non-commutative geometry can shed a new light on monstrous moonshine?

This question is taken up by Jorge Plazas in his paper Non-commutative geometry of groups like $\Gamma_0(N)$

Plazas shows that the bigger Connes-Marcolli $GL_2$ -system also acts on the Big Picture. An intriguing quote:

“Our interest in the $GL_2$ -system comes from the fact that its thermodynamic properties encode the arithmetic theory of modular functions to an extend which makes it possible for us to capture aspects of moonshine theory.”

Looks like the right kind of paper to take along when I disappear next week for some time in the French mountains…

Everything’s wrappable to a sphere

Published January 11, 2018 by lievenlb

One of the better opening quotes of a paper:

“Even quite ungainly objects, like chairs and tables, will become almost spherical if you wrap them in enough newspaper.”

The paper in question is The orbifold notation for surface groups by John Conway.

Here’s Conway talking leisurely about Thurston’s idea to capture the acting group via the topology of the orbifold space and his own notation for such orbifolds.

Here’s another version of the paper, with illustrations: The orbifold notation for two-dimensional groups, by Conway and Daniel H. Huson.

A very accessible account are these lecture notes:

A field guide to the orbifolds, notes from class on “Geometry and the Imagination” in Minneapolis, with John Conway, Peter Doyle, Jane Gilman and Bill Thurston, on June 17–28, 1991.

And, here are notes by Thurston on The Geometry and Topology of Three-Manifolds, including stuff about orbifolds.

I came across these papers struggling my way through On the discrete groups of moonshine by Conway, McKay and Sebbar.

On the genus $0$ property of moonshine groups they have this to say:

“As for groups of the form $(n|h)+e,f,\dots$ , the genus can be determined from the fundamental regions using the Riemann-Hurwitz formula. Since most of the groups are not subgroups of the modular group, the calculations of the genus, which cannot be produced here because of their length, are carried out by finding the elliptic fixed points and the cone points in the orbifolds attached to the fundamental regions. The Euler characteristic of the orbifold determines the genus of the group. See [paper] for more details on orbifold techniques.”

Category: groups

Roots of unity and the Big Picture

nc-geometry and moonshine?

Everything’s wrappable to a sphere