Superintegrability

Table of Contents

Statement

For the simplest case of Gaussian Hermitian matrix model the average of Schur functions is some combo of Schur functions evaluated at some specific points.

(1)

This property generalizes to many more sophisticated cases as well in the symbolic form

(2)

Motivation and overview

To solve matrix model means to calculate all the correlators in this model. This is exactly what we will do in this note! For instance, in the Gaussian case the answer will turn out to be

(3)

where is a partition, sum is taken over partitions and are irreducible characters of symmetric group.

But from the point of view of symmetric functions this answer can be further simplified. The quantity, that is calculated in (3) is actually a correlator of power sum

(4)

But the Frobenius map then enables us to write

(5)

This form is clearly more consice and transparent and hence got its own name.

We can obtain (3) using different methods [MO22] by

  • Wick's theorem
  • using determinant formula for generating function
  • using Itzykson-Zuber as a source in generating function
  • solving Virasoro constraint explicilty

The last two are known to survive -deformation [MO22; Oko97]. Some of these methods are described below.

Wick's theorem

Wick's theorem is the most straightforward way to calculate all the correlators of Gaussian integrals. But this is also the only case when it's simpler to start not with Gaussian Hermitian matrix model, but rather with rectangular complex one (which is also just a product of regular Gaussian integrals, though less symmetric, what will actually simplify some formulae!). See [MM17] and references therein.

Rectangular complex matrix model

Elementary correlators in the rectangular complex matrix model are of form

(6)

where here is not only Young diagram, which characterizes the cycle type of permutation, but rather permutation itself, so the action is defined. and operations should be understood as operations on the permutation's cycle type. is a so-called power power sum.

Wick's theorem for these correlators gives

(7)

By inverse Frobenius map

(8)

we have

(9)

where is an identity matrix. Now,

(10)

We can cook up orthogonality relation for the characters above from Schur orthogonality relations

(11)

Let's multiply them by . We get

(12)

Next, set , and sum over , . We know that , so

(13)

This is exactly the expression we see in (10). Substituting it we obtain

(14)

So we've actually found all the correlators

(15)

By the inverse Frobenius map we have

(16)

and term-by-term comparison of the last two expressions gives

(17)

Gaussian Hermitian matrix model

Wick's theorem is a bit more complicated in this case

(18)

So, all the correlators of this model are then

(19)

Permutations of cycle type are of order 2, i.e. , or , thus in the last product we can sum over with limits . So,

(20)

There are no permutations of order 2 with , therefore

(21)

and we have

(22)

As in complex model we have

(23)

and

(24)

Now, let's get our hands dirty and simplify the last sum. By definition

(25)

so

(26)

Class-sum

(27)

commutes with all elements of since for any we have

(28)

For representation it means the same

(29)

This is exactly the statement of Schur's lemma for , so

(30)

where is identity matrix and is just some number to be found. We proudly substitute this result in (26)

(31)

What remains to do is to find . From (30) we have

(32)

In the last line Frobenius characteristic map was used. Dirty work is done, now back to (24)

(33)

What a beautiful result! Inverse Frobenius characteristic map allows us to obtain

(34)

Itzykson-Zuber source

The starting point is known character expansion for the Itzykson-Zuber integral

(35)

This integral can be used as a source instead of

(36)

so the generating function becomes

(37)

Note, however, that is actually a symmetric function of , so it has the same number of degrees of freedom as our default generating function. The benefit of this kind of source is that can be evaluated independently. For this you need to complete the square

(38)

take Gaussian integral over and trivial integral over (in the calculation of Itzykson-Zuber integral, as well as everywhere else in this notes by default Haar measure is properly normalized)

(39)

The last equality is due to Cauchy identity. From the other hand via character expansion of the Itzykson-Zuber integral we have

(40)

Term-by-term comparison of (39) and (40) gives

(41)

Moreover, by inverse Frobenius characteristic map we have

(42)

References

[MO22]
V. Mishnyakov and A. Oreshina, “Superintegrability in \(\)-deformed Gaussian Hermitian matrix model from \(W\)-operators,” Eur. Phys. J. C, vol. 82, no. 6, p. 548, 2022, doi: 10.1140/epjc/s10052-022-10466-y. arXiv: 2203.15675.
[Oko97]
A. Okounkov, “Proof of a conjecture of goulden and jackson,” Can. J. Math., vol. 49, no. 5, pp. 883–886, 1997, doi: 10.4153/cjm-1997-046-6.
[MM17]
A. Mironov and A. Morozov, “Correlators in tensor models from character calculus,” Phys. Lett. B, vol. 774, pp. 210–216, 2017, doi: 10.1016/j.physletb.2017.09.063. arXiv: 1706.03667.