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Terry Tao RMT book has the following formula for joint moment of freely independent random variables $X,Y$ in Section 2.5

$$\tau(XYXY)=\tau(X)^2\tau(Y^2)+\tau(X^2)\tau(Y)^2-\tau(X)^2\tau(Y)^2$$

Exercise 2.5.17 then asks to prove that this is possible for any joint moment. Is there an easy to describe algorithm for actually constructing such formulas? IE, how would I get $\tau(XYXYXY)$?

I'm looking for procedure I can implement in Mathematica to build a "free probability" version of trace formula table like here

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  • $\begingroup$ I wonder whether the community will some day recognize a subject called "random matrix theory" that somehow includes the study of Wishart matrices. Many books like the cited one by Terrence Tao never mention those, but I wonder whether, among those not belonging to the present-day random matrix community that consumes lots of things like that book, Wishart matrices my be the most well known random matrices. $\endgroup$ Commented Mar 2 at 17:06
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    $\begingroup$ @MichaelHardy The eigenvalues of Wishart matrices are the squares of the eigenvalues of the block matrix that has X in its upper right corner, X^T in the lower left corner, and 0 elsewhere. As such, they are nothing but what is called "Generalized Wigner matrices". Much of the modern theory (including local laws, universality, etc) applies to generalized Wigner matrices. $\endgroup$ Commented Mar 3 at 20:01

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Such "concrete" formulas are addressed in Section 3.4. of my memoir Combinatorial Theory of the Free Product with Amalgamation and Operator-Valued Free Probability Theory. This is in the more general operator-valued context, where the calculations involve nestings of the moments, but of course the same formula is true in the usual scalar-valued case, where everything just factorizes into products. Whether those formulas allow an easy implementation in Mathematica, I don't know, as one has to sum over non-crossing partitions and the appearing coefficients have to be calculated in terms of the Moebius functions (and are, according to Proposition 3.4.2, given by products of signed Catalan numbers).

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  • $\begingroup$ Thanks for the pointer! Wondering if there's a much simpler process for the special case when all individual moments =1 $\endgroup$ Commented Mar 2 at 22:05
  • $\begingroup$ If all moments of X are equal to 1, then X is just the constant 1, so all mixed moments become trivial. $\endgroup$ Commented Mar 3 at 8:52
  • $\begingroup$ Oh right, I meant to ask if there's a much simpler answer for the case of all random variables being independent copies of the same random variable: $d\to \infty$ limit of $d\times d$ Gaussian matrix with $1/\sqrt{d}$ normalization $\endgroup$ Commented Mar 4 at 2:52
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    $\begingroup$ The limit of independent GUE matrices are free semicircular elements. For the calculation in this case, see [my book with Nica] (rolandspeicher.files.wordpress.com/2020/06/…), Example 14.6. (2) $\endgroup$ Commented Mar 5 at 11:59
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Given a collection of free random variables $X_i $, to evaluate a trace of the form $$ \tau [ f_1 (X_{i_1 } ) f_2 (X_{i_2 } ) \ldots f_n (X_{i_n } ) ] $$ where $i_{j+1} \neq i_{j} $, consider the vanishing (by freeness) trace $$ \tau [ (f_1 (X_{i_1 } ) - \tau [f_1 (X_{i_1 }])\ (f_2 (X_{i_2 } ) - \tau [f_2 (X_{i_2 }]) \ldots (f_n (X_{i_n } ) - \tau [f_n (X_{i_n }]) ] = 0 $$ Multiplying this out, one can express the trace of a product of $n$ terms by traces of products of $(n-1)$, $(n-2)$, etc., terms, until the expression is reduced to one containing only individual moments.

Thus (using also cyclicity of the trace), \begin{eqnarray} \tau [XYXY] &=& 2\tau [X] \tau [X Y^2 ] +2\tau [Y] \tau[X^2 Y] -4\tau [X] \tau [Y] \tau [XY] \\ & & {}-(\tau[X])^2 \tau [Y^2 ] -(\tau[Y])^2 \tau [X^2 ]+4(\tau[X])^2 (\tau[Y])^2 \\ & & {}-(\tau[X])^2 (\tau[Y])^2 \\ &=& (\tau [X])^2 \tau [Y^2 ] + (\tau [Y])^2 \tau [X^2 ] -(\tau [X])^2 (\tau [Y])^2 \end{eqnarray} as noted in the OP, and similarly, \begin{eqnarray} \tau [XYXYXY] &=& 3\tau [X] \tau [XYXY^2] + 3\tau [Y] \tau [X^2 YXY] -6\tau [X] \tau [Y] \tau [XYXY] \\ & & {}-3(\tau [X])^2 \tau [XY^3]-3\tau [X] \tau [Y] \tau [X^2 Y^2] -3(\tau [Y])^2 \tau [X^3 Y] \\ & & {}+9(\tau [X])^2 \tau [Y] \tau [XY^2] + 9\tau [X] (\tau [Y])^2 \tau [X^2 Y] +(\tau [X])^3 \tau [Y^3] \\ & & {}+(\tau [Y])^3 \tau [X^3] -9(\tau [X])^2 (\tau [Y])^2 \tau [XY] -3(\tau [X])^3 \tau [Y] \tau [Y^2] \\ & & {}- 3\tau [X] (\tau [Y])^3 \tau [X^2] +6(\tau [X])^3 (\tau [Y])^3 -(\tau [X])^3 (\tau [Y])^3 \end{eqnarray} To evaluate this, we need \begin{eqnarray} \tau [XYXY^2 ] &=& 2\tau [X] \tau [XY^3] + \tau [Y] \tau [X^2 Y^2] +\tau [Y^2 ] \tau [X^2 Y] -2\tau [X] \tau [Y] \tau [XY^2] \\ & & {}- (\tau [X])^2 \tau [Y^3] -2\tau [X] \tau [Y^2 ] \tau [XY] - \tau [Y] \tau [Y^2 ] \tau [X^2 ] \\ & & {}+4(\tau [X])^2 \tau [Y] \tau [Y^2 ] -(\tau [X])^2 \tau [Y] \tau [Y^2 ] \\ &=& (\tau [X])^2 \tau [Y^3] + \tau [Y] \tau [Y^2 ] \tau [X^2 ] -(\tau [X])^2 \tau [Y] \tau [Y^2 ] \end{eqnarray} Inserting this, as well as the expression with $X$ and $Y$ exchanged, and the previous result for $\tau [XYXY]$, we end up with \begin{eqnarray} \tau [XYXYXY] &=& 3\tau [X] \tau [Y] \tau [X^2 ] \tau [Y^2 ] +(\tau [X])^3 \tau [Y^3] +(\tau [Y])^3 \tau [X^3] \\ & & {} -3(\tau [X])^3 \tau [Y] \tau [Y^2] -3(\tau [Y])^3 \tau [X] \tau [X^2] +2(\tau [X])^3 (\tau [Y])^3 \end{eqnarray} This seems feasible to automate (I'd be surprised if it hasn't been, but I don't know where to look).

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