Note: Integral Axioms Values
Steve Trettel
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$\newcommand{\RR}{\mathbb{R}}$
This note concerns the axiomatic description of integration:
An integral on $\RR$ is a choice of set of functions $\mathcal{I}(J)$ for each closed interval $J$ together with a real valued map $\int_J\colon\mathcal{I}(J)\to\RR$ satisfying the following axioms:
If $k\in\RR$ then $f(x)=k$ is an element of $\mathcal{I}([a,b])$ for any interval $[a,b]$ and $$\int_{[a,b]}k = k(b-a).$$
If $f,g\in \mathcal{I}([a,b])$ and $f(x)\leq g(x)$ for all $x\in[a,b]$ then $$\int_{[a,b]}f\leq\int_{[a,b]}g$$
If $[a,b]$ is an interval and $c\in[a,b]$, then $f\in\mathcal{I}([a,b])$ if and only if $f\in\mathcal{I}([a,c])$ and $f\in\mathcal{I}([c,b])$. Furthermore, in this case their values are related by $$\int_{[a,b]}f = \int_{[a,c]}f +\int_{[c,b]}f$$
There are many different integrals by this definition (for example the Riemann/Darboux, Lebesgue, and Gauge integrals). As these axioms do not uniquely specify a function, its a natural question how tight of control they exhibit: can two different integrals agree that a certain function $f$ is integrable, but yet disagree on its value? Precisely, we may ask
Big Question: Let $\int^1,\int^2$ both satisfy the integration axioms, and let $f$ be a function such that $f\in \mathcal{I}_1(J)\cap \mathcal{I}_2(J)$ for some interval $J$. Is it true that $\int^1_J f = \int^2_J f$?
This note provides two first steps towards answering this question. First, we can resolve it for continuous functions, thanks to the Fundamental Theorem of Calculus:
The fundamental theorem of calculus is provable directly from the axioms for continuous functions: if $\int$ is some integral and $f$ is a continuous function that it can integrate on $[a,b]$, then $F(x)=\int_{[a,x]}f$ is differentiable and $F^\prime(x)=f(x)$ (In a previous note, on 2024-05-02).
If $\int^1$ and $\int^2$ are two different integrals for which $f$ is integrable, set $F_1=\int^1_{[a,x]}f$ and $F_2(x)=\int^2_{[a,x]}f$. By the Fundamental theorem, we see $F_1^\prime=F_2^\prime=f$, and so by a corollary to the Mean Value Theorem, since $F_1$ and $F_2$ have the same derivative they differ by a constant. To compute this constant, we need only find $F_2(x)-F_1(x)$ at some point. But since integrals over a singleton are always zero (proven from the axioms in the same note as the Fundamental Theorem), we see
$$F_1(a)=\int_{{a}}^1 f =0\hspace{1cm}F_2(a)=\int_{{a}}^2 f =0$$
Thus $F_2(a)-F_1(a)=0$ and so $F_2(x)=F_1(x)$ for all $x$. Evaluating at $x=b$ yields the result:
$$\int_{[a,b]}^1 f=\int_{[a,b]}^2 f$$
The main theorem of this note extends this to functions which are allowed to be discontinuous on a set of measure zero (proven together in discussions with David Cheng on 2024-08-21)
To prove this result, we can reduce to a simpler statement using the following two well known theorems:
Using these we can reduce the main work to showing that any integral must agree with the Darboux integral when both are defined. Indeed, let $f$ have a measure-zero set of discontinuities. Then $f$ is Riemann, and hence Darboux integrable, so $\int^{\mathrm{Darboux}}f_{[a,b]}$ is defined. If we can show that for any mystery integral $\int^?$ for which $\int^?_{[a,b]}f$ is defined, that $\int^?_{[a,b]}f=\int^{\mathrm{Darboux}}f_{[a,b]}$, we can apply this to any two such integrals $\int^1,\int^2$ for which $f$ is integrable, and conclude
$$\int^1_{[a,b]}f =\int^{\mathrm{Darboux}}_{[a,b]}f= \int^2_{[a,b]}f$$
So we finish the argument by proving this special case, though it is useful to remind ourselves of the definition of the Darboux Integral:
Let $P=P_1\cup P_2\cup \cdots \cup P_n$ be an arbitrary partition of $[a,b]$. Then on each subinterval $P_i$ we know $$m_i=\inf_{P_i}f\leq f(x)\leq\sup_{P_i}f=M_i$$ By subdivision twice (Axiom III) we know that $f$ is $?$-integrable on $P_i$ as it started integrable on $[a,b]$. Because constants are integrable (Axiom I) and we know integration respects inequalities (Axiom II), we can conclude that $$\int_{P_i}m_i\leq \int_{P_i}^?f\leq \int_{P_i}^?M_i$$
Applying the rest of Axiom I (giving the value of the integral of constants), we see $$m_i|P_i|=\int_{P_i}^?m_i\hspace{1cm}M_i|P_i|=\int_{P_i}^?M_i$$ Together this yields bounds on $\int^?_{P_i}f$:
$$m_i|P_i|\leq \int_{P_i}^?f\leq M_i|P_i|$$
Applying subdivision (Axiom III) inductively to the partition $P=P_1\cup\cdots\cup P_n$, $$\int_{[a,b]}^?f = \sum_i \int_{P_i}^?f.$$ Applying the known inequality to each partition gives an inequality on the entire integral: $$\sum_i m_i|P_i|\leq \int_{[a,b]}^? f\leq \sum_i M_i|P_i|$$ But these two bounds are precisely the upper and lower sums of the Darboux integral on $P$. Because we have this inequality for all *arbitrary* partitions $P$, it follows that $$\sup_{P\in \mathcal{P}}\sum_i m_i |P_i|\leq \int_{[a,b]}^?f$$ $$ \int_{[a,b]}^?f\leq \inf_{P\in \mathcal{P}}\sum_i M_i |P_i|$$
Using the assumption that $f$ is Darboux Integrable, we know that the infimum and supremum appearing here are actually equal, and give the value $\int^{\mathrm{Darboux}}_{[a,b]}f$. Thus we’ve squeezed our mystery integral to be exactly this value, as desired:
$$\int_{[a,b]}^?f =\int_{[a,b]}^{\mathrm{Darboux}}f$$