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author | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2020-12-18 16:23:58 +0100 |
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committer | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2020-12-18 16:23:58 +0100 |
commit | 0f62678f523d8a0497c997161e60b3dde61ae83b (patch) | |
tree | 282fad6cdcb94d75c64ca09bf3c82f20995e9d5a | |
parent | a88e086debc8d234f1120f8426384d06408b85fe (diff) | |
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Reassure the reader we are not done.arXiv.v2
-rw-r--r-- | bezout.tex | 7 |
1 files changed, 4 insertions, 3 deletions
@@ -343,9 +343,10 @@ This is, to this order, precisely the Bézout bound, the maximum number of solutions that $N$ equations of degree $p-1$ may have \cite{Bezout_1779_Theorie}. That we saturate this bound is perhaps not surprising, since the coefficients of our polynomial equations -\eqref{eq:polynomial} are complex and have no symmetries. Analogous asymptotic -scaling has been found for the number of pure Higgs states in supersymmetric -quiver theories \cite{Manschot_2012_From}. +\eqref{eq:polynomial} are complex and have no symmetries. Reaching Bézout in +\eqref{eq:bezout} is not our main result, but it provides a good check. +Analogous asymptotic scaling has been found for the number of pure Higgs states +in supersymmetric quiver theories \cite{Manschot_2012_From}. More insight is gained by looking at the count as a function of $a$, defined by $\overline{\mathcal N}(\kappa,\epsilon,a)=e^{Nf(a)}$. In the large-$N$ limit, |