**I.** As a background, in *[Traces of Singular Moduli](http://people.mpim-bonn.mpg.de/zagier/files/tex/TracesSingModuli/fulltext.pdf)* (p.2), Zagier defines the modular form of weight 3/2,


$$g(\tau) = \frac{\eta^2(\tau)}{\eta(2\tau)}\frac{E\_4(4\tau)}{\eta^6(4\tau)}=\vartheta\_4(\tau)\, \eta^2(4\tau)\,\sqrt[3]{j(4\tau)}$$


which has the nice *q*-expansion ([A027652](http://oeis.org/A027652), negated terms),


$$g(\tau) = 1/q - 2 + 248q^3 - 492q^4 +(15^3+744)q^7 + \dots + (5280^3+744)q^{67} + \dots + (640320^3+744)q^{163}+\dots$$


However, one can use other Eisenstein series $E\_k(\tau)$ as the one below.


**II.** In a [paper](http://arxiv.org/pdf/math/0404427v1.pdf) by Bruinier (p.6), Borcherds defines a modular form of weight 1/2. First let,


$$K(\tau) = \tfrac{1}{16}\big(\vartheta\_3^4(\tau) - \tfrac{1}{8}\vartheta\_2^4(\tau)\big)\,\vartheta\_2^4(\tau)\vartheta\_3(\tau)\vartheta\_4^4(\tau)$$


then, 


$$b(\tau) = 60\vartheta\_3(\tau)+\frac{K(\tau)E\_6(4\tau)}{\eta^{24}(4\tau)} = 60\vartheta\_3(\tau)+\frac{K(\tau)\sqrt{j(4\tau)-1728}}{\eta^{12}(4\tau)} $$


This has the *q*-expansion ([A013953](http://oeis.org/A013953)),


$$b(\tau) = 1/q^3 + 4 - 240q + (\color{blue}{27000}-240)q^4 - \color{blue}{85995}q^5 + \color{blue}{1707264}q^8 - (\color{blue}{4096000}+240)q^9 + \color{blue}{44330496}q^{12}-91951146q^{13}+\dots$$


I noticed that the blue numbers appear in the degrees of irreducible representations of the **Thompson group** $Th$, given by the finite sequence of 48 integers ([A003916](http://oeis.org/A003916)),


$$1, 248, 4123, \color{blue}{27000}, 30628, 30875, 61256, \color{blue}{85995}, 147250, 767637, 779247, 957125, \color{blue}{1707264}, 2450240, 2572752, 3376737, \color{blue}{4096000}, 4123000, 4881384, 4936750,\dots\color{blue}{44330496},\dots 91171899, 111321000, 190373976.$$


with repeated terms deleted for brevity.


***Questions***:


1. If it is not coincidence, what is the reason?
2. In Bruinier (p.6) he says one can use $E\_k(\tau)$ for $k=4,6,8,10,14$. What are the other functions for higher $k$?


***Edit***: As pointed out by S. Carnahan below, there is already a known moonshine for $Th$. A partial(?) list of others from Griess' *"Happy Family"* can be found in [Monstrous Moonshine](https://en.wikipedia.org/wiki/Monstrous_moonshine#Generalized_Moonshine), such as for the Higman-Sims $HS$ and so on. (Are there more?)



Monstrous Moonshine for Thompson group $Th$?
This has since been explored and it appears as though there is an interesting type of moonshine for the Thompson group involving weakly holomorphic weight 1/2 modular forms over $\Gamma\_0(N)$ with non-trivial multiplier systems.


To bring out the structure of this moonshine, we can consider the form
\begin{align}
\mathcal{F}\_3(\tau) &\equiv 2b(\tau) + 240\theta(\tau) = \sum\_{\substack{m\geq -3 \\ m\equiv 0,1~\mathrm{mod}~ 4}}c(m)q^m \\
&= 2q^{-3} + 248 + 2\cdot 27000q^4 - 2\cdot 85995q^5 + 2\cdot 1707264 q^8 \\
& \ \ \ \ \ \ \ \ \ \ \ \ \ - 2\cdot 4096000q^9 + 2\cdot44330496q^{12} + \cdots
\end{align}  

where $$\theta(\tau) = \sum\_{n\in \mathbb{Z}}q^{n^2}.$$
Inspection of the character table of Th suggests that we should interpret these first few coefficients as either single, real irreducible representations (with multiplicity 2) or representations of the form $V\oplus \overline{V}$. If we are right in making this association, it might further suggest the existence of a graded module $$W = \bigoplus\_{\substack{m\geq -3 \\ m\equiv 0,1 ~\mathrm{mod}~ 4}}^{\infty}W\_m$$ where we demand that the module be compatible with the Fourier coefficients of $\mathcal{F}\_3$ in the sense that $\dim W\_m = |c(m)|$. The alternating signs can be treated by endowing $W$ with a superspace structure. In other words, we can decompose each component into an odd and even part, $W\_m = W\_m^{(0)} \oplus W\_m^{(1)}$. The multiple of $\theta$ in the definition of $\mathcal{F}\_3$ was chosen so that each Fourier coefficient could be decomposed into dimensions of irreducibles of the same sign. Then, this super-module is special in that, for $m\geq 0$, $W\_m$ has vanishing odd part when $m$ is even and vanishing even part when $m$ is odd. The coefficient of $q^{-3}$ in this sense has the 'wrong sign' in that $W\_{-3}$ has vanishing odd part, a feature similar to one observed in Umbral moonshine.


One can take this idea farther and consider McKay-Thompson series as in Monstrous Moonshine, $$\mathcal{F}\_{3,[g]}(\tau) = \sum \mathrm{str}\_{W\_m}(g)q^m$$ where the $\mathrm{str}$ is meant to denote the super trace. It was found that you can naturally identify these McKay-Thompson series with weight half modular forms (obtained via the formalism of Rademacher series) on $\Gamma\_0(4\cdot o(g)\cdot m)$, i.e. of level 4 times a multiple of the order of $g$, with non-trivial multiplier system. It was verified that these candidates for the McKay-Thompson series produced a well-defined character for the components $W\_m$ for $m\leq 52$. In other words, treating each MT series as a graded character, one can decompose the $W\_m$ into irreducible representations of the Thompson group with positive integer multiplicities for $m\leq 52$ and it is conjecture that this holds more generally for all $m$.


As it turns out, this moonshine is also conjectured to enjoy a discriminant property similar to the one observed in Umbral moonshine, and also has a natural connection to Monstrous moonshine in that the Borcherds lift of $b(\tau)-4\theta(\tau)$ is the $T\_{3C}$ McKay Thompson series from Monstrous moonshine, as was pointed out in earlier comments.


If you'd like to find out more about this moonshine, all this information was taken from the following paper, written by Jeff Harvey and me: <http://arxiv.org/abs/1504.08179>


