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| author | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2018-10-21 23:02:44 -0400 |
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| committer | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2018-10-21 23:02:44 -0400 |
| commit | 3c0d214240facb7e79c8f4953265ca175d928fe3 (patch) | |
| tree | 42e56e262f77fcb167415304959be385e9696299 | |
| parent | bc04424456379aa753d31fbf63ffd8b9bcb6f7e3 (diff) | |
| download | PRE_98_063306-3c0d214240facb7e79c8f4953265ca175d928fe3.tar.gz PRE_98_063306-3c0d214240facb7e79c8f4953265ca175d928fe3.tar.bz2 PRE_98_063306-3c0d214240facb7e79c8f4953265ca175d928fe3.zip | |
no strong statements about exponents!
| -rw-r--r-- | monte-carlo.tex | 6 |
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 |