From ac9061ea00a0722d9b2e55350d08ce264d3e7bfd Mon Sep 17 00:00:00 2001
From: Jaron Kent-Dobias <jaron@kent-dobias.com>
Date: Tue, 21 Nov 2023 17:40:02 +0100
Subject: Added reference to my other paper.

---
 2-point.bib | 14 ++++++++++++++
 2-point.tex |  2 ++
 2 files changed, 16 insertions(+)

diff --git a/2-point.bib b/2-point.bib
index 6fb83bd..60d64cc 100644
--- a/2-point.bib
+++ b/2-point.bib
@@ -403,3 +403,17 @@ Spherical Spin Glasses},
  doi = {10.21468/scipostphys.15.3.109}
 }
 
+@article{Kent-Dobias_2023_When,
+ author = {Kent-Dobias, Jaron},
+ title = {When is the average number of saddle points typical?},
+ journal = {Europhysics Letters},
+ publisher = {IOP Publishing},
+ year = {2023},
+ month = {8},
+ number = {6},
+ volume = {143},
+ pages = {61003},
+ url = {https://doi.org/10.1209%2F0295-5075%2Facf521},
+ doi = {10.1209/0295-5075/acf521}
+}
+
diff --git a/2-point.tex b/2-point.tex
index 5f9bda8..acbba87 100644
--- a/2-point.tex
+++ b/2-point.tex
@@ -213,6 +213,8 @@ are not aware of any result guaranteeing this for the complexity away from the
 ground state, but we check that our replica-symmetric solutions satisfy the
 saddle point equations at {\oldstylenums1}\textsc{rsb}.
 
+\cite{Kent-Dobias_2023_When}
+
 To enforce the spherical constraint at stationary points, we make use of a Lagrange multiplier $\omega$. This results in the extremal problem
 \begin{equation}
   H(\mathbf s)+\frac\omega2(\|\mathbf s\|^2-N)
-- 
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