+- **The nearest visible improvement, and why it is out of reach.** The record above cuts by $\tau\_{\mathfrak{p}\_{13}}^2$, because Proposition 1.8(iii) gives only that the generator of tame inertia $\tau\_{\mathfrak{p}\_{13}}$ has depth *at least* two in $G\_S$. [HMR2019, §3.3.4] observes that if that depth were greater than two, one could cut by $\tau\_{\mathfrak{p}\_{13}}$ itself; the Golod–Shafarevich polynomial would then be at most $1 - 9t + 20t^2 + t^3$, which still has a root in $(0,1)$. The same degree-$12$ field $\mathrm{K}$ would then have an infinite $2$-Hilbert class field tower — no ramification at $13$ needed at all — and the totally real record would fall from $857.567$ to $\mathrm{rd}\_{\mathrm{K}} < 770.644$, a $10\%$ improvement with no new field. The authors write that they “do not see how to check the depth of $\tau\_{\mathfrak{p}\_{13}}$ in $G\_S$”, and [HMR2019, §5.1] raises the general obstruction as Question 5.1: given $S = \\{\mathfrak{p}\\}$ with $\mathfrak{p}$ coprime to $p$ and $G\_S$ infinite, how deep can $\tau\_{\mathfrak{p}}$ be? This is a hope rather than a bound, so nothing in the table above changes; but it is the cheapest known route to the next record.
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