  In this first of two papers, we explain in detail the simplest example of a
broader set of relations between apparently very different theories. Our
example relates $\mathfrak{su}(2)$ $\mathcal{N}=4$ super Yang-Mills (SYM) to a
theory we call "$(3,2)$." This latter theory is an exactly marginal diagonal
$SU(2)$ gauging of three $D_3(SU(2))$ Argyres-Douglas (AD) theories. We begin
by observing that the Schur indices of these two theories are related by an
algebraic transformation that is surprisingly reminiscent of index
transformations describing spontaneous symmetry breaking on the Higgs branch.
However, this transformation breaks half the supersymmetry of the SYM theory as
well as its full $\mathcal{N}=2$ $SU(2)_F$ flavor symmetry. Moreover, it does
so in an interesting way when viewed through the lens of the corresponding 2D
vertex operator algebras (VOAs): affine currents of the small $\mathcal{N}=4$
super-Virasoro algebra at $c=-9$ get mapped to the $\mathcal{A}(6)$ stress
tensor and some of its conformal descendants, while the extra supersymmetry
currents on the $\mathcal{N}=4$ side get mapped to higher-dimensional fermionic
currents and their descendants on the $\mathcal{A}(6)$ side. We prove these
relations are facets of an exact graded vector space isomorphism (GVSI) between
these two VOAs. This GVSI respects the $U(1)_r$ charge of the parent 4D
theories. We briefly sketch how more general $\mathfrak{su}(N)$ $\mathcal{N}=4$
SYM theories are related to an infinite class of AD theories via
generalizations of our example. We conclude by showing that, in this class of
theories, the $\mathcal{A}(6)$ VOA saturates a new inequality on the number of
strong generators.
