quot;. More precisely, for all $\varepsilon>0$, there exists $h=h_{\varepsilon} \in C_{c}^{\infty}(\Omega)$ such that $\|g-h\|_{1}<\varepsilon$. Hence $\|h\|_{1}\geq \|g\|_{1}-\varepsilon. \ \ (*)$Want $\|h\|_{1}$ very small. > > For $\delta>0$, let $h_{\delta}:= \frac{h}{\sqrt{ \delta^{2} + h ^{2} }}$, so that $h_{\delta} \in C^{\infty}_{c}(\Omega)$ and $|h_{\delta}| \leq 1$. ($\delta$ is there to prevent division by zero.) [[Hölder's inequality|Now]], $|\int _{\Omega} \, gh_{\delta}- \int _{\Omega} \, h h_{\delta}|=|\int _{\Omega} (g-h) h _{\delta} \, | \leq \underbrace{ \|g-h\|_{1} }_{ \leq \varepsilon } \underbrace{ \|h_{\delta}\|_{\infty} }_{ \leq 1 } \leq \varepsilon.$By hypothesis, $\int _{\Omega} g h_{\delta} =0$. Also, $|h h_{\delta}| \uparrow |h |$ as $\delta \to 0$. Invoking [[monotone convergence theorem for nonnegative measurable functions|MCT]], we see $\varepsilon \geq \lim_{\delta \to 0} \int _{\Omega} | h h_{\delta} | \, = \int _{\Omega} |h| \, d\mu =\|h\|_{1}.$ > Combining with $(*)$, gives $\|g\|_{1} \leq 2 \varepsilon$ for all $\varepsilon>0$, and the result follows. > ---- #### ----- #### References > [!backlink] > ```dataview > TABLE rows.file.link as "Further Reading" > FROM [[]] > FLATTEN file.tags as Tag > WHERE Tag = "#definition" OR Tag = "#theorem" OR Tag = "#MOC" OR Tag = "#proposition" OR Tag = "#axiom" > GROUP BY Tag > ``` > [!frontlink] > ```dataview > TABLE rows.file.link as "Further Reading" > FROM outgoing([[]]) > FLATTEN file.tags as Tag > WHERE Tag = "#definition" OR Tag = "#theorem" OR Tag = "#MOC" OR Tag = "#proposition" OR Tag = "#axiom" > GROUP BY Tag > ```