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Question: Give an example of a Borel measurable function ${f: [0,1]^2 \rightarrow {\bf R}}$ such that the integrals ${\int_{[0,1]} f(x,y)\,\mathrm dy}$ and ${\int_{[0,1]} f(x,y)\,\mathrm dx}$ exist and are absolutely integrable for all ${x \in [0,1]}$ and ${y \in [0,1]}$ respectively, and that ${\int_{[0,1]} \left(\int_{[0,1]} f(x,y)\,\mathrm dy\right)\,\mathrm dx}$ and ${\int_{[0,1]} \left(\int_{[0,1]} f(x,y)\,\mathrm dx\right)\,\mathrm dy}$ exist and are absolutely integrable, but such that $$ \int_{[0,1]} \left(\int_{[0,1]} f(x,y)\,\mathrm dy\right)\,\mathrm dx \neq \int_{[0,1]} \left(\int_{[0,1]} f(x,y)\,\mathrm dx\right)\,\mathrm dy$$ are unequal. (Hint: adapt the doubly infinite sequence ${(x_{n,m})_{n,m \in {\bf N}}}$ such that ${x_{n,m}}$ equals ${+1}$ when ${n=m}$, ${-1}$ when ${n=m+1}$, and ${0}$ otherwise.) Thus we see that Fubini’s theorem fails when one drops the hypothesis that ${f}$ is absolutely integrable with respect to the product space.

Attempt: Partition the unit interval $[0,1]$ into $\left[\frac{1}{2^{k-1}}, \frac{1}{2^k}\right)$, $k=1, 2, \ldots$ as countably many sub-intervals of length $2^{-k}$. Denote by $I_n$ the $n^{\text{th}}$ interval in the $x$-axis, and $J_m$ the $m^{\text{th}}$ interval in the $y$-axis. Define $f:[0,1]^2 \rightarrow {\bf R}$ by $$f(x,y) := \sum_{n,m} x_{n,m} 1_{I_n \times J_m}(x,y).$$ It then seems that $$\int_{[0,1]} \left(\int_{[0,1]} f(x,y)\,\mathrm dy\right)\,\mathrm dx = \frac{1}{2} \neq 0 = \int_{[0,1]} \left(\int_{[0,1]} f(x,y)\,\mathrm dx\right)\,\mathrm dy.$$ But how about the part that emphasizes the absolute integrability of $f$ w.r.t. the product space?

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    $\begingroup$ I do not think your example gives a counterexample of the Fubini's Theorem as for your $f$, $|f|\le 1$ and therefore $\int_{[0,1]^2} |f|$ is finite, which satisfies the hypothesis of Fubini's Theorem. In order to adapt the example of sequence $(x_{n,m})$ in the hint, one should not set $f$ to be $x_{n,m}$ on $I_n\times J_m$. Instead one should construct $f$ so that its integration on $I_n\times J_m$ equals $x_{n,m}$. $\endgroup$ Commented yesterday
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    $\begingroup$ A minor remark: In Measure Theory, there is no such thing as an absolutely integrable function. Any integrable function is an absolutely integrable. $\endgroup$ Commented yesterday
  • $\begingroup$ @KaviRamaMurthy: All relevant definitions are from Terry Tao’s “An Introduction to Measure Theory” textbook. $\endgroup$ Commented yesterday

2 Answers 2

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Take the famous example

$$f(x,y)=\frac{x^{2}-y^{2}}{(x^{2}+y^{2})^{2}}$$

Then $\int_{0}^{1}f(x,y)\,dy=\frac{1}{1+x^{2}}$ (As $\frac{d}{dy}\frac{y}{x^{2}+y^{2}}=f(x,y)$)

which gives you $\int_{0}^{1}(\int_{0}^{1}f(x,y)dy)dx=\frac{\pi}{4}$.

On the other hand, $\int_{0}^{1}f(x,y)\,dx=-\frac{1}{1+y^{2}}$ and hence $\int_{0}^{1}(\int_{0}^{1}f(x,y)\,dx)\,dy)=-\frac{\pi}{4}$.


Where does this function fail Fubini's conditions?

It's because the function is not integrable (absolutely integrable) wrt the Lebesgue measure on $[0,1]^{2}$. To see this, restrict to the unit disc and use polar coordinates to say

\begin{align}\iint_{[0,1]^{2}}|\frac{x^{2}-y^{2}}{(x^{2}+y^{2})^{2}}|&\,d(x,y)\geq\iint_{x^{2}+y^{2}\leq 1}|\frac{x^{2}-y^{2}}{(x^{2}+y^{2})^{2}}|\,d(x,y)\\\\ &=\int_{0}^{2\pi}\int_{0}^{1}\frac{r^{2}|\cos^{2}(\theta)-\sin^{2}(\theta)|}{r^{4}}\cdot r\,dr\,d\theta=+\infty \end{align}

As also mentioned in the comments, for Lebesgue integrals, absolute integrability and integrability are the same things and Lebesgue integral is only defined for absolutely integrable functions.

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  • $\begingroup$ Thanks, an edited solution is posted using the original hint of the problem. $\endgroup$ Commented 13 hours ago
  • $\begingroup$ @shark Yeah that's the standard infinite matrix example that works easily with the counting measure on $\Bbb{N}\times\Bbb{N}$. i.e. $x_{i,i}=1$, $x_{i,i+1}=-1$ for each $i$ and $x_{i,j}=0$ otherwise. Then the row sums are $0$ identically and thus the row-column sum is 0. But the column-row sum is $1$. $\endgroup$ Commented 6 hours ago
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Let ${(x_{n,m})_{n,m \in {\bf N}}}$ be a doubly infinite sequence of extended non-negative reals such that ${x_{n,m}}$ equals ${+1}$ when ${n=m}$, ${-1}$ when ${n=m+1}$, and ${0}$ otherwise. Now, partition the unit interval $[0,1]$ into $[\frac{1}{2^{k-1}}, \frac{1}{2^k}),\ k=1, 2, \ldots$ as countably many sub-intervals of length $2^{-k}$. Denote by $I_n$ the $n^{th}$ interval in the $x$-axis, and $J_m$ the $m^{th}$ interval in the $y$-axis. Define $f:[0,1]^2 \rightarrow {\bf R}$ by \begin{align*} f(x,y) := \sum_{n,m} \frac{x_{n,m}}{|I_n| \cdot |J_m|} 1_{I_n \times J_m}(x,y). \end{align*} $\forall x \in [0,1],\ f(x,y) = \frac{1}{|I_n|} \sum_{m} \frac{x_{n,m}}{|J_m|} 1_{J_m}(y)$ for some fixed $n$. Specifically, \begin{align*} g(x) := \int_{[0,1]} f(x,y)\ dy = \begin{cases} 2, & x \in I_1 \\ 0, & x \in I_n\ \text{for}\ n \geq 2 \end{cases} \end{align*} Hence $g(x)$ is integrable, and we have \begin{align*} \int_{[0,1]} (\int_{[0,1]} f(x,y)\ dy)\ dx = \int_{[0,1]} g(x)\ dx = 1. \end{align*} $\forall y \in [0,1],\ f(x,y) = \frac{1}{|J_m|} \sum_{n} \frac{x_{n,m}}{|I_n|} 1_{I_n}(x)$ for some fixed $m$. Specifically, \begin{align*} h(y) := \int_{[0,1]} f(x,y)\ dx = 0. \end{align*} Hence $h(y)$ is integrable, and we have \begin{align*} \int_{[0,1]} (\int_{[0,1]} f(x,y)\ dx)\ dy = \int_{[0,1]} h(y)\ dy = 0. \end{align*} The function $f$ as defined is clearly Borel-measurable. But \begin{align*} |f(x,y)| = \sum_{n,m} \frac{1}{|I_n| \cdot |J_m|} 1_{I_n \times J_m}(x,y) \end{align*} is not integrable with respect to the product space.

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