ON THE FOURIER COEFFICIENTS OF WORD MAPS ON UNITARY GROUPS 3
When w=xℓ, (1.2) gives a formula for the moments of traces, and one can use Newton’s identities
relating elementary symmetric polynomials and power sums, to deduce that
Ecm(Xℓ)2=E|tr (Symmw)|2=ℓ+m−1
m,
for d≥2mℓ (see Appendix A). In [Rai97, Rai03], Rains partially extended (1.2) for small dand gave
an explicit formula for the joint density of the eigenvalues of Xℓ(see [Rai03, Theorem 1.3]).
We now move to general words w∈Fr. The case m= 1, namely, the asymptotics as d→ ∞ of the
distribution of the random variable tr (w(X1,...,Xr)), was studied in the context of Voiculescu’s free
probability (see e.g. [VDN92, MS17]). In particular, in [Voi91, R˘
06, MSS07] it was shown that, for
a fixed w∈Fr, the sequence of random variables tr (w(X1,...,Xr)), for d= 1,2,..., converges in
distribution, as d→ ∞, to a complex normal random variable (with suitable normalization). As a
direct consequence, for a fixed m∈N, the random variables cm(w(X1,...,Xr)) converge, as d→ ∞,
to a certain explicit polynomial of Gaussian random variables. This is done in Appendix A, Corollary
A.4, following [DG06].
In [MP19], Magee and Puder have shown that E(tr (w(X1,...,Xr))) coincides with a rational function
of d, if dis sufficiently large, and bounded its degree in terms of the commutator length of w. They
also found a geometric interpretation for the coefficients of the expansion of that rational function as
a power series in d−1, see [MP19, Corollaries 1.8 and 1.11]. See [Bro24] for additional work in this
direction.
1.2. Ideas of proofs. With a few exceptions, the results stated in §1.1 are asymptotic in d, but not
uniform in both mand d. We will try to explain some of the challenges in proving results that are
uniform in m, while explaining the idea of the proof of Theorem 1.1.
Our main tool (which is also used in the papers [R˘
06, MSS07, MP19] above) to study integrals on
unitary groups is the Weingarten Calculus ([Wei78, Col03, CS06]). Roughly speaking, the Weingarten
Calculus utilizes the Schur–Weyl Duality to express integrals on unitary groups as sums of so called
Weingarten functions over symmetric groups. In our case, in order to prove Theorem 1.1, we need to
estimate the integral
(1.3) E|cm(w)|2=ZUr
dtr ^mw(X1,...,Xr)2dX1. . . dXr.
Using Weingarten calculus (Theorem 2.12), we express (1.3) as a finite sum
(1.4) X
(π1,...,π2r)∈Q2r
i=1 Smℓi
F(π1,...,π2r)
r
Y
i=1
Wg(i)
d(πiπ−1
i+r),
where ℓ1,...,ℓ2r∈Nand F:Q2r
i=1 Smℓi→Zare related to combinatorial properties of w, and each
Wg(i)
d:Smℓi→Ris a Weingarten function (see Definition 2.10). There are two main difficulties when
dealing with sums such as (1.4) in the region when mis unbounded:
(1) While the asymptotics of Weingarten functions Wgd:Sm→Rare well understood when
d≫m(see [Col03, Section 2.2] and [CM17, Therem 1.1]), much less is known in the regime
where mis comparable with d.
(2) Even if we have a good understanding of a single Weingarten function, the number of sum-
mands in (1.4) is large and it is not enough to bound each individual Weingarten function.
Luckily, there are plenty of cancellations in the sum (1.4). To understand these cancellations, we
identify a symmetry of (1.4). More precisely, we find a group Hacting on Q2r
i=1 Smℓisuch that Fis