From 3c0d214240facb7e79c8f4953265ca175d928fe3 Mon Sep 17 00:00:00 2001
From: Jaron Kent-Dobias <jaron@kent-dobias.com>
Date: Sun, 21 Oct 2018 23:02:44 -0400
Subject: no strong statements about exponents!

---
 monte-carlo.tex | 6 +++---
 1 file changed, 3 insertions(+), 3 deletions(-)

(limited to 'monte-carlo.tex')

diff --git a/monte-carlo.tex b/monte-carlo.tex
index f5ff8e7..76a4103 100644
--- a/monte-carlo.tex
+++ b/monte-carlo.tex
@@ -618,9 +618,9 @@ of $hL^{\beta\delta/\nu}$.
     model-dependent. Colored lines and points depict values as measured by the
     extended algorithm. Solid black lines show a plot proportional to
     $h^{-z\nu/\beta\delta}$ for each model. The dynamic exponents $z$ are
-    roughly measured as \twodee Ising: 0.23(2), \threedee Ising: 0.28(2),
-    \twodee 3-State Potts: 0.55(1), \twodee 4-State Potts: 0.94(5),
-    \threedee O(2): 0.17(2), \threedee O(3): 0.13(2). $\mathrm O(n)$ models
+    roughly measured as \twodee Ising: 0.23(5), \threedee Ising: 0.28(5),
+    \twodee 3-State Potts: 0.55(5), \twodee 4-State Potts: 0.94(5),
+    \threedee O(2): 0.17(5), \threedee O(3): 0.13(5). $\mathrm O(n)$ models
     use the distribution of transformations described in Section
     \ref{sec:examples:on}. The curves stop collapsing at high fields when the
     correlation length falls to near the lattice spacing; here non-cluster
-- 
cgit v1.2.3-54-g00ecf

