$\DeclareMathOperator\Rep{Rep}$It is well-known that the Macdonald "$P$" polynomials deform the Jack "$J$" polynomials [1]. The latter have profound relations with representation theory. For example, setting $\alpha=1$ on $J$ recovers the Schur polynomials; setting $\alpha=2$ on $J$ recovers the zonal polynomials (related to Gelfand pairs, Selberg $\alpha$-integral…); setting $\alpha=(-1)$ almost recovers the monomial symmetric polynomial. Given such results, it is clear that Macdonald "$P$" polynomials must also have profound meaning in representation theory. Indeed, this has been long pursued using several methods: DAHA, equivariant K-theory, geometric of Hilbert schemes, generalized intertwiners. Some combinatorial interpretations have also been found (c.f. Ram and Yip - A combinatorial formula for Macdonald polynomials, ASEP, etc).
In this thread I'm mainly interested in seeing a more direct relation with the symmetric groups $S_{d}$. In short, how do Macdonald polynomials hint about $(q,t)$-deforming the symmetric groups $S_{d}$ (or their group algebras, or their representation categories…)?
Frobenius Formula and Symmetric Functions
Let us start by recalling the relation between the symmetric groups and the Jack polynomials. Let $V_{\lambda}$ be the irreducible representation of $S_{d}$ corresponding to the partition $\lambda$. This induces a character $\chi^{\lambda}$ whose values are of interest. Since characters are class functions, it is enough to look at its values on the set of conjugacy classes of $S_{d}$, which is parametrized by partitions
$$\mu = (d,d,\dotsc,d,d-1,d-1,\dotsc,2,1,1,\dotsc,1),$$
with $\sum_{i} \mu_{i} = d$. The answer is beautifully given by the Frobenius formula [2]. Here's a concise formulation:
$$p_{\mu} = \sum_{\lambda} \chi^{\lambda}({\mu}) s_{\lambda},$$
where $p$ denotes the power-sum symmetric polynomials and $s$ denotes the Schur symmetric polynomials. In other words, the transformation matrices between the power-sum symmetric functions and the Schur symmetric functions are given by the characters in $\Rep(S_{\infty})$!
Jack Polynomials and $\alpha$-deformation
Now let's recall how Jack polynomials are defined in [1]. Construct an inner product $(,)$ on a suitable ring such that
$$(s_{\lambda}, s_{\mu}) = \delta_{\lambda,\mu}.$$
Then the $p$'s also form an orthogonal basis: $$(p_{\lambda}, p_{\mu}) = \delta_{\lambda,\mu} z_{\lambda}$$ for some scalar $z_{\lambda}$. Moreover, the Frobenius formula says that the character values are given by $(p_{\mu}, s_{\lambda})$.
Now, deforming the inner product to $(,)_{\alpha}$ by requiring
$$(p_{\lambda}, p_{\mu})_{\alpha} = \delta_{\lambda,\mu} z_{\lambda} \alpha^{l(\lambda)},$$
we then have the Jack polynomials as a certain orthogonal basis under this deformed pairing.
Question
By the Frobenius formula and the definition of the Jack's polynomial, it seems that there should be a way to $\alpha$-deform $\Rep(S_{\infty})$ such that the character values are given by $(p_{\mu}, s_{\lambda})_{\alpha}$.
Can one deform $\Rep(S_{\infty})$ further so that the character values are given by $(p_{\mu}, s_{\lambda})_{(q,t)}$, where the pairing (this gives the Macdonald functions) is given by deforming $\alpha^{l(\lambda)}$ to $\prod_{i=1}^{\lambda} \frac{1-q^{\lambda_{i}}}{1-t^{\lambda_{i}}}$. This question is asked essentially in [3].
Reference
[1] Symmetric Functions and Hall Polynomials-[Macdonald]
[2] Representation Theory-[Fulton and Harris]
[3] Generalization of Frobenius formula involving Macdonald polynomials