In this note we study two point functions of Coulomb branch chiral ring elements with
large R-charge, in quantum field theories with N = 2 superconformal symmetry in four
spacetime dimensions. Focusing on the case of one-dimensional Coulomb branch, we use
the effective-field-theoretic methods of [1], to estimate the two-point correlation function
Yn ≡ |x − y|2n∆O(O(x))n(O¯(y))n�in the limit where the operator insertion On has large
total R-charge J = n∆O. We show that Yn has a nontrivial but universal asymptotic
expansion at large J , of the form Yn = J !�|NO|2π�2JJα Y˜n ,where Y˜
n approaches a constant as n → ∞, and NO is an n-independent constant describing
on the normalization of the operator relative to the effective Abelian gauge coupling.
The exponent α is a positive number proportional to the difference between the a-anomaly
coefficient of the underlying CFT and that of the effective theory of the Coulomb branch.
For Lagrangian SCFT, we check our predictions for the logarithm Bn = log(Yn), up to and
including order log(J ) against exact results from supersymmetric localization [2–5]. In the
case of N = 4 we find precise agreement and in the case N = 2 we find reasonably good
numerical agreement at J ' 60 using the no-instanton approximation to the S
4 partition
function. We also give predictions for the growth of two-point functions in all rank-one SCFT
in the classification of [6–9]. In this way, we show the large-R-charge expansion serves as a
bridge from the world of unbroken superconformal symmetry, OPE data, and bootstraps, to
the world of the low-energy dynamics of the moduli space of vacua
