Abstract
Abstract
We consider
$$ \mathcal{N} $$
N
= 2 SU(N) SQCD in four dimensions and a weak-coupling regime with large R-charge recently discussed in arXiv:1803.00580. If φ denotes the adjoint scalar in the
$$ \mathcal{N} $$
N
= 2 vector multiplet, it has been shown that the 2-point functions in the sector of chiral primaries (Trφ
2)
n
admit a finite limit when g
YM → 0 with large R-charge growing like ∼ 1/g
YM
2
. The correction with respect to
$$ \mathcal{N} $$
N
= 4 correlators is a non-trivial function F(λ; N) of the fixed coupling λ = n g
YM
2
and the gauge algebra rank N. We show how to exploit the Toda equation following from the tt
* equations in order to control the R-charge dependence. This allows to determine F(λ; N) at order
$$ \mathcal{O} $$
O
(λ10) for generic N, greatly extending previous results and placing on a firmer ground a conjecture proposed for the SU(2) case. We show that a similar Toda equation, discussed in the past, may indeed be used for the additional sector (Trφ
2)
n
Trφ
3 due to the special mixing properties of these composite operators on the 4-sphere. We discuss the large R-limit in this second case and compute the associated scaling function F at order
$$ \mathcal{O} $$
O
(λ
7) and generic N. Large N factorization is also illustrated as a check of the computation.
Publisher
Springer Science and Business Media LLC
Subject
Nuclear and High Energy Physics
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