A General Discussion
In analytic number theory, the nature of an arithmetic function $f:\mathbb{N}\rightarrow\mathbb{R}$ is studied in many different ways, like
- Studying the growth of the summatory function $F:\mathbb{R}_{\geq1}\rightarrow\mathbb{R}$ defined as follows $$F(x):=\sum_{n\leq x}f(n)$$
- Studying frequency of values $f(n),n\in\mathbb{N}$ among the reals by considering the function $\mathcal{F}:\mathbb{R}_{\geq1}\rightarrow\mathbb{R}$ defined as follows$$\mathcal{F}(x):=|\{f(n):f(n)\leq x\}|$$
- Finding functions $f_1:\mathbb{R}\rightarrow\mathbb{R}$ such that $$f(n)\sim f_1(n)$$ or $$f(n)=O(f_1(n))$$
Results regarding the number of unordered factorizations of an integer
It's an interesting question in analytic number theory to study the number of unordered factorizations of a positive integer. Many results regarding this are known and this is still an active field of research.
Let us define the function for formally stating some of the important results. For a positive integer, $n$ let $\psi(n)$ denote the number of tuples $(n_1,n_2,\ldots,n_k)$ such that $1<n_1\leq n_2\leq\cdots\leq n_k$ and $n=n_1n_2\cdots n_k$. This function was first studied comprehensively by A. Oppenheim. He proved that
$$\sum_{n\leq x}\psi(n)\sim\frac{xe^{2\sqrt{\log(x)}}}{2\sqrt{\pi}(\log(x))^{3/4}}\tag{1}$$ For more details read the following paper
[Opp] A. Oppenheim, On an arithmetic function, J. London Math. Soc.1(1926), 205-211; part II in2(1927),123-130.
In some recent developments, the following function is studied,
$$\Psi(x):=|\{\psi(n):\psi(n)\leq x\}|$$ for $x\geq1$. R. Balasubramanian and Priyamvad Srivastav proved the following,
Theorem Let $C=2\pi\sqrt{2/3}$, then for sufficiently large $x$ we have $$\Psi(x)\leq\exp\left(C\sqrt{\frac{\log(x)}{\log(\log(x))}}\left(1+O\left(\frac{\log(\log(\log(x)))}{\log(\log(x))}\right)\right)\right)\tag{2}$$
For more details read the following paper
arXiv:1609.08602v1 [math.NT] 27 Sep 2016 ON THE NUMBER OF FACTORIZATIONS OF AN INTEGER
Some interesting special cases
For a prime $q$ and $n\geq1$, $\psi(q^n)$ is exactly equal to the number of unordered partitions of $n$ with positive integral parts. Therefore $$\psi(q^n)=p(n)$$ where $p(\cdot)$ is the well-known partition function.
For $n=p_1p_2\cdots p_r$ being a square-free positive integer with $r$ distinct prime factors, $\psi(n)$ is the same as the number of partitions of a set of $r$ distinct elements which is known as the $r^{th}$ Bell number and denoted as $B_r$. Therefore $$\psi(n)=B_r$$ for square-free $n$ with $r$ distinct prime factors.