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| author | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2024-10-29 13:59:40 +0100 |
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| committer | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2024-10-29 13:59:40 +0100 |
| commit | 79309cd70841ecc1a0c34776ab962785c1e6ebce (patch) | |
| tree | 774d94f413afb01ac99f14cb8e14a3945cac6326 | |
| parent | 8b2218dbcb8b05059312fa7741e5510c0ca077f2 (diff) | |
| download | marginal-79309cd70841ecc1a0c34776ab962785c1e6ebce.tar.gz marginal-79309cd70841ecc1a0c34776ab962785c1e6ebce.tar.bz2 marginal-79309cd70841ecc1a0c34776ab962785c1e6ebce.zip | |
Wording tweak.
| -rw-r--r-- | marginal.tex | 2 |
1 files changed, 1 insertions, 1 deletions
diff --git a/marginal.tex b/marginal.tex index 3e89bd7..1f1143c 100644 --- a/marginal.tex +++ b/marginal.tex @@ -669,7 +669,7 @@ for typical samples $H$. In particular, here we study only cases with quadratic $g_i$, which results in a linear expression relating $\mu$ and the $\omega_i$ that is independent of $\mathbf x$. Since $H$ contains the disorder of the problem, this simplification means -that the effect of fixing the trace is independent of the disorder and only +that the effect of fixing the trace is largely independent of the disorder and mostly depends on properties of the constraint manifold. \subsection{Superspace representation} |