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-rw-r--r--monte-carlo.tex6
1 files changed, 3 insertions, 3 deletions
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