TITLE: Why did Voiculescu develop free probability?
QUESTION [24 upvotes]: I was recently asked why Voiculescu developed free probability theory. I am not very expert in this and the only answer I was able to provide is the classical one: he was challenging the isomorphism problem of whether $II_1$-factors associated to two different free groups are isomorphic or not. First: is this true or just legend? Were there any other motivations? In particular I would be interested in more down-to-earth motivations, something that could theoretically be explained to someone with basic knowledge in probability theory and operator theory (without necessarily knowing what a $II_1$-factor is).
Thanks in advance!
Valerio

REPLY [12 votes]: Here is a more detailed account on the history by Dan Voiculescu himself. This is from his article "Background and Outlook" in the Lectures Notes
"Free Probability and Operator Algebras", see
http://www.ems-ph.org/books/book.php?proj_nr=208

Just before starting in this new direction, I had worked with Mihai Pimsner,
  computing the K-theory of the reduced $C^*$-algebras of free groups. From the
  K-theory work I had acquired a taste for operator algebras associated with free
  groups and I became interested in a famous problem about the von Neumann
  algebras $L(\mathbb{F}_n)$ generated by the left regular representations of free groups,
  which appears in Kadison's Baton-Rouge problem list. The problem, which
  may have already been known to Murray and von Neumann, is:are $L(\mathbb{F}_m)$ and $L(\mathbb{F}_n)$ non-isomorphic if $m \not= n$?
This is still an open problem. Fortunately, after trying in vain to solve it,
  I realized it was time to be more humble and to ask: is there anything I can
  do, which may be useful in connection with this problem? Since I had come
  across computations of norms and spectra of certain convolution operators on
  free groups (i.e., elements of $L(\mathbb{F}_n)$), I thought of finding ways to streamline
  some of these computations and perhaps be able to compute more complicated
  examples. This, of course, meant computing expectations of powers of such
  operators with respect to the von Neumann trace-state $\tau(T) = \langle T e_e,e_e\rangle$, $e_g$
  being the canonical basis of the $l^2$-space.
The key remark I made was that if $T_1$, $T_2$ are convolution operators on $\mathbb{F}_m$
  and $\mathbb{F}_n$ then the operator on $\mathbb{F}_{m+n} = \mathbb{F}_m \ast \mathbb{F}_n$ which is $T_1 + T_2$, has moments $\tau((T_1 + T_2)^p)$ which depend only on the moments $\tau(T_j^k)$, $j = 1, 2$ , but not
  on the actual $T_1$ and $T_2$. This was like the addition of independent random
  variables, only classical independence had to be replaced by a notion of free
  independence, which led to a free central limit theorem, a free analogue of
  the Gaussian functor, free convolution, an abstract existence theorem for one
  variable free cumulants, etc.