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As a term of a Serre spectral sequence, I would like to compute the cohomology group with compact support $H^*_c(\mathcal{M}_{1,[2]},\mathbb{V}_1)$ of the moduli space of genus $1$ curves with $2$ unordered marked points, with values in $\mathbb{V}_1$, the standard representation of $SL_2(\mathbb{Z})$, coming from the cohomology group $H^1(E,\mathbb{Q})$, where $E$ is an elliptic curve.

I know that $H^*_c(\mathcal{M}_{1,1},\mathbb{V}_1)=0$, and I would like to try to use this result to obtain a similar one for the case of $2$ unordered marked points.

My attempt so far consists in using mapping class groups, the Birman exact sequence

\begin{equation*} 1\to \pi_1(S_{1,1})\to \text{PMod}(S_{1,2})\to \text{PMod}(S_{1,1})\to 1 \end{equation*} and the Hochschild-Serre spectral sequence of group cohomology, to obtain $H^*(\mathcal{M}_{1,2},\mathbb{V}_1)$ (which I believe to be identically $0$), using the fact that the action of the fibre $\pi_1(S_{1,1})\cong \mathbb{Z}*\mathbb{Z}$ on the local system is trivial, as $\mathbb{V}_1$ is a representation of $\text{PMod}(S_{1,1})\cong SL_2(\mathbb{Z})$.

Since I am not used to mapping class groups and group cohomology, I have, now, two questions:

  1. Is the reasoning so far correct?
  2. Assuming it is, this takes care only of the moduli stack $\mathcal{M}_{1,2}$ with ordered points. How do I obtain the cohomology of the unordered one? I think that would consist in getting rid of the action of the elliptic involution, exchanging the marked points, but it is not clear to me how to effectively do it.

To be coherent with other results I have, I would hope this cohomology groups not to be identically $0$.

I would appreciate any comment on my problem, or any helpful reference for the computation of $H^*_c(\mathcal{M}_{1,[2]},\mathbb{V}_1)$, also with other methods.

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1 Answer 1

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Your approach is good but you must have messed something up with the Hochschild-Serre spectral sequence.

I prefer the sheafy approach over thinking about the Hochschild-Serre spectral sequence, so let me explain it in these terms. So we have the forgetful map $\pi : M_{1,2} \to M_{1,1}$, and we may write $$ H^\bullet_c(M_{1,2},V) = H^\bullet_c(M_{1,1},R\pi_!V ).$$ Now $V=\pi^\ast V$ is actually pulled back from $M_{1,1}$ and we have $$R\pi_! \pi^\ast V \cong (R\pi_!\mathbf Q) \otimes V \cong (V \otimes V)[-1] \oplus V(-1)[-2]$$ where in the first step we used the projection formula and in the second we used a section to split $R\pi_!\mathbf Q$ in the derived category. Representation theory of $\mathrm{SL}(2)$ shows that $V \otimes V \cong V_2 \oplus \mathbf Q(-1)$, where $V_2$ is the second symmetric power of $V$ and $\mathbf Q(-1)$ is a Tate twist of the trivial representation. From the Eichler-Shimura isomorphism we know $H^\bullet_c(M_{1,1},-)$ with coefficients taken in all of these summands: $H^2_c(M_{1,1},\mathbf Q(-1)) \cong \mathbf Q(-2)$, $H^1_c(M_{1,1},V_2)\cong \mathbf Q(0)$, all other cohomologies vanish. So $H^\bullet_c(M_{1,2},V)$ is $\mathbf Q(-2)$ in degree $3$, $\mathbf Q(0)$ in degree $2$, and vanishes otherwise.

To deal with unordered points we use that $H^\bullet_c(M_{1,[2]},V) = H^\bullet_c(M_{1,2},V)^{\Sigma_2}$, where $\Sigma_2$ acts by permuting the markings. Unfortunately the computation in the previous paragraph isn't immediately $\Sigma_2$-equivariant. But in fact $\Sigma_2$ acts on $M_{1,2}$ preserving the map $\pi$; it acts by multiplication by $-1$ on the universal elliptic curve. To see this we consider a curve with two marked points $(x,y)$. We can translate to make the first coordinate the origin, and our markings are then $(0,y-x)$. Clearly if we had swapped $x$ and $y$ we would have gotten $x-y$ instead. Inversion in $V$ acts as the identity on $V \otimes V$, so $H^\bullet_c(M_{1,[2]},V) = H^\bullet_c(M_{1,2},V)$.

Hope this is coherent with other results you have!

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  • $\begingroup$ Thank you for your precise and quick answer! I indeed care about Tate twists too. On that note, could you please explain how did you obtain those? I would assume $H^2_c(M_{1,1},\mathbb{Q})\cong\mathbb{Q}(-1)$ already, but I can't see how to deduce the twists on $H^k_c(M_{1,2},V)$. $\endgroup$
    – Marco Fava
    Commented Mar 23, 2023 at 9:36
  • $\begingroup$ OK! I put them in. $\endgroup$ Commented Mar 23, 2023 at 13:05
  • $\begingroup$ You mentioned that to split $R\pi_!\mathbf Q$ in corresponding derived category one have to use certain section. Could you lose few words on why such section in the setting above must always exist? $\endgroup$
    – JackYo
    Commented Apr 25, 2023 at 20:17
  • $\begingroup$ I was being very sloppy and careless. To split it, it's enough to have a multisection of degree 1 on each fiber, so you could e.g. take 1/3 times the sum of the 2-torsion points on your elliptic curves. Or you could work with a continuous section rather than an algebraic section. Or you could simply ignore trying to split $R\pi_!\mathbf Q$ in the derived category; for our purposes it's enough that the Leray-Serre spectral sequence degenerates, which is obvious in this case as there is no room for a nonzero differential on the $E_2$ page. $\endgroup$ Commented Apr 26, 2023 at 16:06
  • $\begingroup$ The last argument with LS-spectral seq of course works but I would like to understand better this first splitting approach, since I'm not sure if I completely got it. So far we want to get a split of $R\pi_!\mathbf Q$, the naive approach is to to find a splitting of a distinguished triangle carrying $R\pi_!\mathbf Q$ as middle term. If such dist triangle comes from a "geometric" morphism $f: X \to S$ like in our case with $\pi$, then the "classical" trick from homological algebra to obtain a split is to find a section of $f$. $\endgroup$
    – JackYo
    Commented Apr 28, 2023 at 23:19

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