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@@ -41,7 +41,7 @@ For the general case,
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By the Monotone Convergence Theorem (use $|f|\chi_{[-N,N]}$ to approximate $|f|$), we can find $N$ large such that
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By the Monotone Convergence Theorem (use $|f|\chi_{[-N,N]}$ to approximate $|f|$), we can find $N$ large such that
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$$
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$$
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\int_{E_N^c}|f|dm<\frac{\epsilon}{2}
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\int_{E_N^c}|f|dm<\frac{\epsilon}{3}
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$$
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$$
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where $E_N=E\cap [-N,N]$.
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where $E_N=E\cap [-N,N]$.
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@@ -54,8 +54,72 @@ $$
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\int_{E_N} |f-\phi|dm<\frac{\epsilon}{3}
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\int_{E_N} |f-\phi|dm<\frac{\epsilon}{3}
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$$
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$$
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For each $i=1,2,\cdots,n$, we can find $g_i$ continuous such that
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$$
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\int_{E}|\chi_{S_i}-g_i|dm<\frac{\epsilon}{3M}
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$$
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where $M=\sum_{i=1}^n |\alpha_i|$.
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Take $g=\sum_{i=1}^n \alpha_i g_i$,
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$$
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\int_E |\phi-g|dm\leq \sum_{i=1}^n |\alpha_i|\int_E |g_i-\chi_{S_i}|dm<\frac{\epsilon}{3}
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$$
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$\phi-g=\sum_{i=1}^n \alpha_i (\chi_{S_i-g_i})$
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All in all,
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$$
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\begin{aligned}
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\int_E |f-g|dm&\leq \int_E|f-\phi|dm+\int_E |\phi-g|dm\\
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&=\int_{E_N^c}|f|dm+\int_E |f-\phi|dm+\int_E |\phi-g|dm\\
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&<\frac{\epsilon}{3}+\frac{\epsilon}{3}+\frac{\epsilon}{3}\\
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&=\epsilon
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\end{aligned}
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$$
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QED
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QED
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### Road map for proving the fundamental theorem of calculus in Lebesgue integration
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Recall the Riemann-Stieltjes integral:
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If $g\in \mathscr{R}(\alpha)$ on $[a,b]$,
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$G(x)=\int_a^x g d\alpha$,
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then:
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1. $G$ is continuous on $[a,b]$
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2. If $g$ is continuous at $x\in [a,b]$, then $G$ is differentiable at $x$ with $G'(x)=g(x)$.
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To extend this to the case where $g$ is Lebesgue integrable, we use the Hardy-Littlewood maximal function.
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#### Definition of the Hardy-Littlewood maximal function
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Given an interval $I\subseteq \mathbb{R}$, define the averaging operator $A_I f(x)=\frac{\chi_I(x)}{m(I)}\int_I f(x)dm$.
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(This function takes the average of $f$ over the interval $I$.)
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The Hardy-Littlewood maximal function is defined as:
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$$
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f^*(x)=\sup_{I\text{ is open interval}}A_I f(x)
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$$
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We will show that $f^*$ is not that such worse than $f$. (Prove on Wednesday)
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Relates to the Fundamental Theorem of Calculus in Lebesgue integration.
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$$
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\frac{G(x+h)-G(x)}{h}=\frac{1}{h}\int_x^{x+h} g(t)dt=A_{[x,x+h]}g(x)
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$$
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If we can control all the averages, we can control the function.
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pages/Math4121/Math4121_L38.md
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pages/Math4121/Math4121_L38.md
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pages/Math4121/Math4121_L39.md
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pages/Math4121/Math4121_L39.md
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@@ -39,4 +39,8 @@ export default {
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Math4121_L33: "Introduction to Lebesgue Integration (Lecture 33)",
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Math4121_L33: "Introduction to Lebesgue Integration (Lecture 33)",
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Math4121_L34: "Introduction to Lebesgue Integration (Lecture 34)",
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Math4121_L34: "Introduction to Lebesgue Integration (Lecture 34)",
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Math4121_L35: "Introduction to Lebesgue Integration (Lecture 35)",
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Math4121_L35: "Introduction to Lebesgue Integration (Lecture 35)",
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Math4121_L36: "Introduction to Lebesgue Integration (Lecture 36)",
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Math4121_L37: "Introduction to Lebesgue Integration (Lecture 37)",
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Math4121_L38: "Introduction to Lebesgue Integration (Lecture 38)",
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Math4121_L39: "Introduction to Lebesgue Integration (Lecture 39)",
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}
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}
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pages/Math416/Math416_L26.md
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pages/Math416/Math416_L26.md
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@@ -0,0 +1 @@
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pages/Math416/Math416_L27.md
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pages/Math416/Math416_L27.md
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@@ -0,0 +1 @@
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@@ -29,4 +29,6 @@ export default {
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Math416_L23: "Complex Variables (Lecture 23)",
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Math416_L23: "Complex Variables (Lecture 23)",
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Math416_L24: "Complex Variables (Lecture 24)",
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Math416_L24: "Complex Variables (Lecture 24)",
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Math416_L25: "Complex Variables (Lecture 25)",
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Math416_L25: "Complex Variables (Lecture 25)",
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Math416_L26: "Complex Variables (Lecture 26)",
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Math416_L27: "Complex Variables (Lecture 27)",
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}
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}
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