Generalized Breuil–Mézard conjecture for GLn\operatorname{GL}_n

Let KK be a finite extension of Qp\mathbb Q_p, let rˉ:GKGLn(F){\bar{r}}:G_K\to\operatorname{GL}_n(\mathbb F) be continuous, and let Rrˉ,λ,τR^\square_{{\bar{r}},\lambda,\tau} be the potentially crystalline deformation ring of Hodge type λ\lambda and inertial type τ\tau. If (Lλ,τOF)ssaFana(L_{\lambda,\tau}\otimes_{\mathcal O}\mathbb F)^{\operatorname{ss}}\cong\bigoplus_a F_a^{n_a}, where aa ranges over Serre weights, then Generalized Breuil–Mézard conjecture. There exist integers μa(rˉ)\mu_a({\bar{r}}) depending only on rˉ{\bar{r}} and aa such that

e(Rrˉ,λ,τ/π)=anaμa(rˉ).e(R^\square_{{\bar{r}},\lambda,\tau}/\pi)=\sum_a n_a\mu_a({\bar{r}}).

This is the higher-dimensional analogue of the Breuil–Mézard conjecture, expressing deformation-ring multiplicities through Serre-weight data.

Sources & referencesView supporting material

Primary source

Matthew Emerton and Toby Gee, “A geometric perspective on the Breuil-Mézard conjecture”, arXiv:1109.4226 (2013).

Progress summary

Never refreshed

Nothing recorded yet. Refresh searches the literature and the public web for attempts on this problem, and writes the first summary here.

Solutions 0

No solutions have been posted yet.