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| author | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2021-03-18 21:49:13 +0100 |
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| committer | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2021-03-18 21:49:13 +0100 |
| commit | 5a903b3dca614142434a51054157e1f6642a63ae (patch) | |
| tree | 79ee8463b45dbfb3562f6b8c4f6e2ba215cb5543 | |
| parent | 0107fa065ab055dcd724aad1cf87c2146e31ec88 (diff) | |
| download | PRR_3_023064-5a903b3dca614142434a51054157e1f6642a63ae.tar.gz PRR_3_023064-5a903b3dca614142434a51054157e1f6642a63ae.tar.bz2 PRR_3_023064-5a903b3dca614142434a51054157e1f6642a63ae.zip | |
Missing word added.
| -rw-r--r-- | bezout.tex | 2 |
1 files changed, 1 insertions, 1 deletions
@@ -101,7 +101,7 @@ One might balk at the constraint $z^Tz=N$---which could appropriately be called a \emph{hyperbolic} constraint---by comparison with $z^\dagger z=N$. The reasoning behind the choice is twofold. -First, we seek draw conclusions from our model that are applicable to generic +First, we seek to draw conclusions from our model that are applicable to generic holomorphic functions without any symmetry. Samples of $H_0$ nearly provide this, save for a single anomaly: the value of the energy and its gradient at any point $z$ correlate along the $z$ direction, with $\overline{H_0\partial |