diff options
author | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2021-06-16 17:56:03 +0200 |
---|---|---|
committer | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2021-06-16 17:56:03 +0200 |
commit | 08047f31e51e25c764622630d22b01dd404d80ec (patch) | |
tree | a807c6c3efeb3427ad17cd52852252abaedcbc26 /stokes.tex | |
parent | f92bd7967eab5ed5fd62c74d9b876066804bf5e1 (diff) | |
download | JPA_55_434006-08047f31e51e25c764622630d22b01dd404d80ec.tar.gz JPA_55_434006-08047f31e51e25c764622630d22b01dd404d80ec.tar.bz2 JPA_55_434006-08047f31e51e25c764622630d22b01dd404d80ec.zip |
Added plot of ground state.
Diffstat (limited to 'stokes.tex')
-rw-r--r-- | stokes.tex | 35 |
1 files changed, 35 insertions, 0 deletions
@@ -372,6 +372,41 @@ imaginary energy join. H_p=\frac1{p!}\sum_{i_1\cdots i_p}J_{i_1\cdots i_p}z_{i_1}\cdots z_{i_p} \end{equation} +\begin{figure} + \begin{gnuplot}[terminal=epslatex, terminaloptions={size 8.65cm,5.35cm}] + set parametric + set hidden3d + set isosamples 100,25 + set samples 100,100 + unset key + set dummy u,r + set urange [-pi:pi] + set vrange [1:1.5] + set cbrange [0:2] + set xyplane 0 + + set xlabel '$\operatorname{Re}\epsilon$' + set ylabel '$\operatorname{Im}\epsilon$' + set zlabel '$r$' + set cblabel '$\frac\epsilon{\epsilon_{\mathrm{th}}}$' + + p = 4 + set palette defined (0 "blue", 0.99 "blue", 1.0 "white", 1.01 "red", 2 "red") + set pm3d depthorder border linewidth 0.5 + + s(r) = sqrt(0.75 * log(9 * r**4 / (1 + r**2 + r**4)) / (8 * r**4 - r**2 - 1)) + x(u, r) = cos(u) * s(r) * sqrt(1 + 5 * r**2 + 5 * r**4 + r**6) + y(u, r) = sin(u) * s(r) * sqrt((r**2 - 1)**3) + thres(u, r) = ((x(u,r) / (r**(p - 2) + 1))**2 + (y(u,r) / (r**(p - 2) - 1))**2) / ((p - 1) / (2 * p * r**(p - 2))) + + splot "++" using (x(u, r)):(y(u, r)):2:(thres(u, r)) with pm3d lc palette + \end{gnuplot} + \caption{ + The surface of extant states for the 4-spin model, that is, those for which + the complexity is zero. + } +\end{figure} + \subsection{(2 + 4)-spin} \begin{equation} |