Fredrik said:
On second thought, it looks like this isn't over yet. At the end of the argument, we have to be able to conclude that since V(G) is finite, ##\mu(G)## is finite. This relies on the earlier claim "For all ##A\in\Sigma## such that ##\mu(A)=\infty##, we have ##V(A)=\infty##". But can we really prove that, without making assumptions about what sort of subsets A has?
I'm starting to think that we have to assume at least this: For all M>0, every set of infinite measure has a subset of finite measure greater than M.
Don't all interesting measure spaces satisfy this condition anyway?
Yes, for sure.
Alright, here is a counterexample:
Consider ##X=\mathbb{R}##, consider all sets measurable and let ##\mu(A) = +\infty## for each nonempty ##A\subseteq X## and of course ##\mu(\emptyset) = 0##.
Clearly, ##\mathcal{S}= \{0\}##.
Consider the function ##f = \chi_\mathbb{R}##. Let ##\mathcal{I}=\{\alpha f~\vert~\alpha\in \mathbb{R}\}##. Define ##\phi(g) = 0## for each ##g\in \mathcal{I}##. This satisfies all the conditions, but Chebyshev is not satisfied. The function is also not integrable in your sense.
We can eliminate this case either by demanding
(1) There is no measurable subset ##E## of ##X## such that each subset of ##E## either has infinite measure or measure ##0## and such that the measure ##E## is infinite.
(2) Add to the axioms of ##\mathcal{I}## and ##\phi## that if ##g_n\in \mathcal{S}## with ##g_n = 0## a.e., then the limit (if it exists) of the ##g_n## under ##rho## is zero a.e.
(3) Add to the axioms that if ##\rho(f)=0##, then ##f=0## a.e. This is similar to (2).
Let's prove that either of those conditions is enough to prove Chebyshev, and thus your theorem.
So take ##h## integrable and ##A = \{x~\vert~h(x)>a\}##. It is easy to see that
V(A) = \textrm{sup}\{\mu(F)~\vert~F\subseteq A,~\mu(F)<+\infty\}
So assume that ##V(A)## is finite but that ##\mu(A)## is infinity, then there exists a sequence ##F_n\subseteq A## such that ##\mu(F_n)<+\infty## and such that ##\mu(F_n)\rightarrow V(A)##. We can easily make the sequence increasing, thus we have that ##\mu(\bigcup_n F_n) = V(A)##. So there is a set ##F## of measure ##V(A)##.
Let's look at ##A\setminus F##. Then this has infinite measure. Assume that it contains a set of finite measure ##B##. Then ##\mu(F\cup B) = \mu(F) + \mu(B)\geq V(A)##. Thus follows that ##B## has measure ##0##. So all subsets of ##A\setminus F## either have measure ##0## or measure infinity. If we accepted ##(1)## as true, then ##\mu(A\setminus F) = 0##, and thus ##\mu(A) = \mu(F)## has finite measure. Contradiction.
In the other case that ##(2)## or ##(3)## is true, we have found a subset ##E\subseteq A## of infinite measure such that each subset has either measure ##0## or measure infinity.
Consider ##\mathcal{I}^\prime = \{f\chi_E~\vert~f\in \mathcal{I}\}##. This can be seen as a quotient space of the vector space ##\mathcal{I}## under the map ##P:\mathcal{I}\rightarrow \mathcal{I}^\prime:f\rightarrow f\chi_E##. In particular, it has a canonical seminorm
\rho^\prime(f^\prime) = \textrm{inf}\{\rho(f)\in \mathcal{I}~\vert~f\chi_E = f^\prime\}
Since ##\mathcal{S}## is dense in ##\mathcal{I}##. It follows that ##\{g\chi_E~\vert~g\in \mathcal{S}\}## is dense in ##\mathcal{I}^\prime##. But clearly, any integrable function is almost everywhere ##0## on ##E##. Thus if ##g\in \mathcal{S}##, then ##g\chi_E = 0## a.e. Thus ##\rho(g) = 0## for each ##g\in \mathcal{I}^\prime##.
But since ##A = \{x~\vert~h(x)>a\}##. We have that ##h\chi_E>a##. Thus there exists a sequence ##(g_n)_n## in ##\mathcal{S}^\prime## such that ##g_n\rightarrow h\chi_E## in ##\rho^\prime##. Since ##g_n=0## a.e., it follows from ##(2)##that ##h\chi_E = 0## a.e, which contradicts ##h\chi_E>a##.
If ##(3)## is true, then it follows from ##\rho(g)=0## for each ##g\in \mathcal{I}^\prime## that ##h\chi_E = 0## a.e. which contradicts again ##h\chi_E>a##.