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| author | Juan Marin Noguera <juan@mnpi.eu> | 2022-12-04 22:49:17 +0100 |
|---|---|---|
| committer | Juan Marin Noguera <juan@mnpi.eu> | 2022-12-04 22:49:17 +0100 |
| commit | c34b47089a133e58032fe4ea52f61efacaf5f548 (patch) | |
| tree | 4242772e26a9e7b6f7e02b1d1e00dfbe68981345 /gae/n5.lyx | |
| parent | 214b20d1614b09cd5c18e111df0f0d392af2e721 (diff) | |
Oops
Diffstat (limited to 'gae/n5.lyx')
| -rw-r--r-- | gae/n5.lyx | 16 |
1 files changed, 8 insertions, 8 deletions
@@ -149,7 +149,7 @@ Fijado \end_inset dada por -\begin_inset Formula $\ell(\vec{v}):=\overrightarrow{f(A)f(A+\vec{v})}$ +\begin_inset Formula $\ell(\vec{v})\coloneqq \overrightarrow{f(A)f(A+\vec{v})}$ \end_inset es lineal, entonces @@ -200,11 +200,11 @@ A continuación veamos que \end_inset , si -\begin_inset Formula $P:=A+\vec{v}$ +\begin_inset Formula $P\coloneqq A+\vec{v}$ \end_inset y -\begin_inset Formula $Q:=A+\vec{w}$ +\begin_inset Formula $Q\coloneqq A+\vec{w}$ \end_inset , deducimos @@ -441,7 +441,7 @@ simetría ortogonal con deslizamiento \end_inset , siendo -\begin_inset Formula $A:=\frac{Q+f(Q)}{2}$ +\begin_inset Formula $A\coloneqq \frac{Q+f(Q)}{2}$ \end_inset para @@ -473,7 +473,7 @@ En efecto, dado \end_inset y llamamos -\begin_inset Formula $A:=\frac{Q+f(Q)}{2}=Q+\frac{1}{2}(\vec{v}+\vec{w})$ +\begin_inset Formula $A\coloneqq \frac{Q+f(Q)}{2}=Q+\frac{1}{2}(\vec{v}+\vec{w})$ \end_inset , como @@ -709,11 +709,11 @@ Sea . Sean ahora -\begin_inset Formula $g:=t_{-\vec{v}}\circ f$ +\begin_inset Formula $g\coloneqq t_{-\vec{v}}\circ f$ \end_inset y -\begin_inset Formula ${\cal H}:=Q+F^{\bot}$ +\begin_inset Formula ${\cal H}\coloneqq Q+F^{\bot}$ \end_inset . @@ -789,7 +789,7 @@ status open \end_inset Sea -\begin_inset Formula $g:=\rho_{\ell,\theta}$ +\begin_inset Formula $g\coloneqq \rho_{\ell,\theta}$ \end_inset , para un |
