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author | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2022-06-10 11:39:36 +0200 |
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committer | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2022-06-10 11:39:36 +0200 |
commit | eabaacdec785dd3d02c9147d2b635d6e1564a28d (patch) | |
tree | 91fd057b216e301e2a2bbe603153968376396e15 | |
parent | 1e2aea428aeb56acc378d01e014b59b8ae6fff42 (diff) | |
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Killed extra space.
-rw-r--r-- | frsb_kac_new.tex | 2 |
1 files changed, 1 insertions, 1 deletions
diff --git a/frsb_kac_new.tex b/frsb_kac_new.tex index 4d938da..44fce5b 100644 --- a/frsb_kac_new.tex +++ b/frsb_kac_new.tex @@ -376,7 +376,7 @@ We shall make the following ansatz for the saddle point: D_{ab}= D_d \delta_{ab} \end{align} From what we have seen above, this means that replica $a$ is insensitive to -a small field applied to replica $b$ if $a \neq b$, a property related to ultrametricity. A similar situation happens in quantum replicated systems, +a small field applied to replica $b$ if $a \neq b$, a property related to ultrametricity. A similar situation happens in quantum replicated systems, with time appearing only on the diagonal terms: see Appendix C for details. From its very definition, it is easy to see just perturbing the equations |