Undergrad On translation and dilation invariant Lebesgue measure: Folland's text

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The discussion centers on the translation and dilation invariance of Lebesgue measure as outlined in Folland's text. It confirms that if a set E belongs to the Lebesgue σ-algebra, then both E translated by s and E dilated by r also belong to this σ-algebra, with measures m(E+s) and m(rE) being equal to m(E) and |r|m(E), respectively. The author clarifies how to demonstrate these properties for finite unions of intervals, emphasizing that the measure of an interval is simply its length. By showing that translations and dilations preserve the structure of disjoint unions, the conclusion is reached that the measure remains consistent under these transformations. Overall, the invariance of Lebesgue measure under translation and dilation is effectively validated through these arguments.
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I am stuck at a claim made in Theorem 1.21 in Folland's real analysis text on the translation and invariant Lebesgue measure on ##\mathbb R##.
Let ##m## be Lebesgue measure and ##\mathcal L## the Lebesgue ##\sigma##-algebra (the complete ##\sigma##-algebra that includes the Borel ##\sigma##-algebra). Consider,

Theorem 1.21. If ##E\in\mathcal L##, then ##E+s\in\mathcal L## and ##rE\in \mathcal L## for all ##s,r\in \mathbb R##. Moreover, ##m(E+s)=m(E)## and ##m(rE)=|r|m(E)##.

Folland starts off by saying that the collection of open intervals is invariant under translations and dilations, so the same is true for ##\mathcal B_\mathbb{R}##. I understand that claim; basically consider ##\mathcal B'=\{E\in\mathcal B_\mathbb{R}:E+t\in\mathcal B_\mathbb{R},t\in\mathbb R\}## and show it's a ##\sigma##-algebra that contains all the open intervals and hence ##\mathcal B_\mathbb{R}##, and by definition, ##\mathcal B'\subset \mathcal B_\mathbb{R}##. So ##\mathcal B'=\mathcal B_\mathbb{R}##. Same for dilations.

However, then he goes on to say that if we let ##m_s(E)=m(E+s)## and ##m^r(E)=m(rE)## for ##E\in \mathcal B_\mathbb{R}##, then they "clearly" agree with ##m## and ##|r|m## on finite unions of intervals. This claim I don't understand. If we define ##\phi_t(x)=x+t## as the translation by ##t##, and if ##A## is a finite union of intervals, then $$\phi_t(A)=\phi_t\left(\bigcup_{n=1}^N E_n\right) = \bigcup_{n=1}^N \phi_t(E_n).$$ But how do I show ##m_s(A)=m(A)##? The thing that's confusing me is that up until now, he has only talked about finite disjoint union of h-intervals, where an h-interval is a set of the form ##(a,b]##, ##(a,\infty)## or ##\varnothing## for ##-\infty\leq a<b<\infty##. I'm sure his statement is correct as it stands, but I don't know how to show ##m_s(A)=m(A)##.
 
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What's the measure of (a,b] + s = (a + s, b+ s]?
What's the measure of r(a,b] = \begin{cases}<br /> (ra, rb] &amp; r &gt; 0 \\<br /> (0,0] &amp; r = 0 \\<br /> [rb, ra) &amp; r &lt; 0 \end{cases}
 
Thanks @pasmith! I'll just add this here as an answer to my question.

The author notes prior to the theorem that the Lebesgue measure of an interval is just its length, so if ##I## is an interval with endpoints ##a,b## with ##a<b##, its measure is ##b-a##. Clearly ##m_s(I)=m(I)## and ##m^r(I)=|r|m(I)##. And if ##A=\bigcup_1^n I_i## where ##I_i## are intervals, then first observe that we can make them disjoint and obtain ##A=\bigcup_1^k J_j##. Disjoint is preserved under translation and dilation, so if ##\phi_s(x)=x+s## (the very same argument applies to ##\phi_r(x)=rx##), it follows that \begin{align*}m_s(A)&=m(\phi_s(A))=m\left(\phi_s\left(\bigcup_{j=1}^k J_j\right)\right)= m\left(\bigcup_{j=1}^k \phi_s(J_j)\right)=\sum_1^k m(\phi_s(J_j))\\ &=\sum_1^k m_s(J_j)=\sum_1^k m(J_j)=m\left(\bigcup_{j=1}^kJ_j\right)=m(A).\end{align*} Thus ##m_s(E)=m(E)## and ##m^r(E)=|r|m(E)## for ##E## being a finite union of intervals.
 
We all know the definition of n-dimensional topological manifold uses open sets and homeomorphisms onto the image as open set in ##\mathbb R^n##. It should be possible to reformulate the definition of n-dimensional topological manifold using closed sets on the manifold's topology and on ##\mathbb R^n## ? I'm positive for this. Perhaps the definition of smooth manifold would be problematic, though.

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