Something a little odd - Lebesgue vs Riemann integral

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The discussion centers on the differences between the Riemann and Lebesgue integrals, particularly regarding the improper integral of the function f(x) = sin(x). It establishes that the Riemann integral over the entire real line does not equal the limit of the integral over symmetric intervals, while the Lebesgue integral allows for a different approach using signed measures. Specifically, the Lebesgue integral can be defined as the limit of integrals over increasing measurable sets, which can yield different results than the Riemann approach when dealing with non-integrable functions like sin(x).

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quasar987
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In the Riemann theory for a function f defined on all of R, we define its improper integral over R as the sum of two limits:

\int_{-\infty}^{+\infty}f(x)dx = \lim_{a\rightarrow -\infty}\int_{a}^0f(x)dx+\lim_{b\rightarrow +\infty}\int_{0}^b f(x)dx

and in general, this is not equal to

\lim_{L\rightarrow +\infty}\int_{-L}^L f(x)dx

For instance, for f(x)=sin(x), neither of the two limits above exists, but the limit below is 0.

But what does Lebesgue says? We know that given f:R-->R integrable, the function \nu:\mathfrak{L}_{\mathbb{R}}\rightarrow \mathbb{R} defined by

\nu(E)=\int_Ef(x)dx

is a (signed) measure. Signed measures enjoy the same continuity properties as finite and positive measures. That is, if E_n is an increasing sequence of measurable sets, then

\nu\left(\bigcup_{n=1}^{+\infty}E_n\right)=\lim_{n\rightarrow +\infty}\nu(E_n)

In particular, for E_n = ]-n,n[ and the measure defined above,

\int_{-\infty}^{+\infty}f(x)dx=\lim_{n\rightarrow +\infty}\int_{-n}^nf(x)dx

(Since U E_n=R)

What's up with that? (as in : any comments welcome)
 
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quasar987 said:
In the Riemann theory for a function f defined on all of R, we define its improper integral over R as the sum of two limits:

\int_{-\infty}^{+\infty}f(x)dx = \lim_{a\rightarrow -\infty}\int_{a}^0f(x)dx+\lim_{b\rightarrow +\infty}\int_{0}^b f(x)dx

and in general, this is not equal to

\lim_{L\rightarrow +\infty}\int_{-L}^L f(x)dx

For instance, for f(x)=sin(x), neither of the two limits above exists, but the limit below is 0.

But what does Lebesgue says? We know that given f:R-->R integrable, the function \nu:\mathfrak{L}_{\mathbb{R}}\rightarrow \mathbb{R} defined by

\nu(E)=\int_Ef(x)dx

is a (signed) measure. Signed measures enjoy the same continuity properties as finite and positive measures. That is, is E_n is an increasing sequence of measurable sets, then

\nu\left(\bigcup_{n=1}^{+\infty}E_n\right)=\lim_{n\rightarrow \infty}\nu(E_n)

In particular, for E_n = ]-n,n[ and the measure defined above,

\int_{-\infty}^{+\infty}f(x)dx=\lim_{n\rightarrow +\infty}\int_{-n}^nf(x)dx

(Since U E_n=R)

What's up with that? (as in : any comments welcome)
With that choice of E_n, you are doing, effectively,
\lim_{n\rightarrow \infty}\int_{-n}^{n} f(x) dx[/itex]<br /> the &quot;Cauchy Principal Value&quot;, <b>not</b> the general Lebesque integral.
 
Explain please!

What would the general Lebesgue integral be?
 
i seem to recall the lebesgue integral subtracts the negative part of the integral from the positive one (i.e. does the integrals of max(f,0) and min(f,0) separately) so you would simply get a non integrable function for sin since both integrals are infinite. but i have not looked at this in 40 years.
 
It would be using a sequence of measurable sets that was NOT symmetric as you have it.

Just after I read your question, I then asked myself the question you are probably thinking of: in order to be integrable, it shouldn't MATTER which measurable sets we choose! That's true but it is also true of Riemann integrable functions (in terms of intervals rather than measurable sets).

Note that
\lim_{L\rightarrow \infty}\int_{-L}^L f(x)dx= \lim_{a\rightarrow -\infty}\int_a^0 f(x)dx \lim_{b\rightarrow\infty}\int_0^L f(x)dx
is true if all the integrals exist.

In terms of the Lebesque integral, just as for the Riemann integral, even if
\int_{-\infty}^{+\infty}f(x)dx=\lim_{n\rightarrow +\infty}\int_{-n}^nf(x)dx
exists the "more general" integral,, using other measurable sets may not exist.
 
mathwonk spotted my error: sin(x) is not Lebesgue integrable because |sinx| isn't.

It would be nice then, if we could show that if f 's improper Riemann integral diverges, then it isn't Lebesgue integrable. This way, we then never encounter the humbling situation

\int_{-\infty}^{+\infty}f(x)dx \ \ \ \mbox{(Riemann)} \neq\lim_{L\rightarrow +\infty}\int_{-L}^L f(x)dx \ \ \ \mbox{(Riemann)} = \int_{-\infty}^{+\infty}f(x)dx \ \ \ \mbox{(Lebesgue)}

Bed.
 
I don't understand your dilemma. If a function is Riemann integrable, then the Riemann and Lebesgue integrals agree on any bounded interval, right? And isn't it a straightforward proof that

\int_{-\infty}^{+\infty} f(x) \, dx = \lim_{<br /> \substack{a \rightarrow -\infty \\ b \rightarrow +\infty }}<br /> \int_a^b f(x) \, dx

whenever either side exists? (for both kinds of integrals)
 

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