I am currently taking a course on probability theory for mathematicians where we're doing some measure theory. I've been thinking about how it is that if $\mathcal{L}$ is a $\lambda$-system and a $\pi$-system, then $\mathcal{L}$ is a $\sigma$-algebra (the converse is very straightforward).
Before explaining what I mean, I should point out that we have taken the following definition of $\lambda$-system. $\mathcal{L} \in \mathcal{P}(\Omega) $ is a $\lambda$-system iff
- $\Omega \in \mathcal{L}$
- $A, B \in \mathcal{L}$ and $A \subseteq B \Rightarrow B \setminus A \in \mathcal{L}$
- $A_1, A_2, \ldots \in\mathcal{L}$ such that $A_n \uparrow A \Rightarrow A \in \mathcal{L}$
Suppose $\mathcal{L}$ is a $\lambda$-system. For $\mathcal{L}$ to be a $\sigma$-algebra, in addition to the easy-to-check fact that for any set in $\mathcal{L}$, its complement is also in $\mathcal{L}$, the enumerable union of an arbitrary collection of sets in $\mathcal{L}$ must also be in $\mathcal{L}$. So I started by taking two arbitrary sets.
Let $A, B \in \mathcal{L}$. Suppose $D_1 = A, D_j = A \cup B, \forall j \in \mathbb{N}-\{1\}$. Then $D_1 \subseteq D_2 \subseteq D_3 \subseteq \ldots $ and clearly $\cup_{j \in \mathbb{N}} D_j = A \cup B$. This would mean that $D_j \uparrow (A \cup B)$, so property $(3)$ above would imply that $A \cup B \in \mathcal{L}$.
But then if I already had this for two sets, I could generalize for finite unions. Moreover, if $A_1, A_2, \ldots \in L$, then $$\bigcup\limits_{j=1}^n A_j \uparrow \bigcup\limits_{j=1}^\infty A_j. $$ Again, property $(3)$ would imply that $\bigcup\limits_{j=1}^\infty A_j \in \mathcal{L}$.
Clearly there is something wrong, since not all $\lambda$-systems are $\sigma$-algebras. I would really appreciate that you point out any mistakes in the reasoning above.