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| author | kurchan.jorge <kurchan.jorge@gmail.com> | 2020-12-09 13:06:52 +0000 | 
|---|---|---|
| committer | overleaf <overleaf@localhost> | 2020-12-09 13:06:53 +0000 | 
| commit | 930eb0fd79ce8b0960e86d2b190f4333f1457d82 (patch) | |
| tree | b9503aa968253e947936617ca4fe7bd4651d1704 | |
| parent | 3b1b4f32a709b87769436c5e0922f3ebf22fe9fd (diff) | |
| download | PRR_3_023064-930eb0fd79ce8b0960e86d2b190f4333f1457d82.tar.gz PRR_3_023064-930eb0fd79ce8b0960e86d2b190f4333f1457d82.tar.bz2 PRR_3_023064-930eb0fd79ce8b0960e86d2b190f4333f1457d82.zip  | |
Update on Overleaf.
| -rw-r--r-- | bezout.tex | 2 | 
1 files changed, 1 insertions, 1 deletions
@@ -330,7 +330,7 @@ Consider for example the ground-state energy for given $a$, that is, the energy  {\color{teal} {\bf somewhere} In Figure \ref{desert} we show that for $\kappa<1$ there is always a range of values of $a$ close to one for which there are no solutions: this is natural, given that the $y$ contribution to the volume shrinks to zero as that of an $N$-dimensional sphere $\sim(a-1)^N$.  For the case $K=1$ -- i.e. the analytic continuation of the usual real computation -- the situation -is more interesting. In the range of  values of $$ +is more interesting. In the range of  values of $\Re$  \begin{figure}[htpb]\label{desert}  | 
