Abstract
We compute the one-point functions of chiral primary operators in the non-supersymmetric defect conformal field theory that is dual to the IIB string theory on $AdS_5\times S^5$ background with a probe D7 brane with internal gauge field flux, both in perturbative Yang-Mills theory and in the string theory dual. The former is expected to be accurate at weak coupling whereas the latter should be accurate in the planar strong coupling limit of the gauge theory. We consider the distinct cases where the D7 brane has geometry $AdS_4\times S^4$ with an instanton bundle of the worldvolume gauge fields on $S^4$ and $AdS_4\times S^2\times S^2$ with Dirac monopole bundles on each $S^2$. The gauge theory computation and the string theory computation can be compared directly in the planar limit and then a subsequent limit where the worldvolume flux is large. We find that there is exact agreement between the two in the leading order.
Highlights
Probe branes and defect conformal field theories have been widely studied in the context of AdS/CFT holography [1]-[23]
We compute the one-point functions of chiral primary operators in the nonsupersymmetric defect conformal field theory that is dual to the IIB string theory on AdS5 × S5 background with a probe D7 brane with internal gauge field flux, both in perturbative Yang-Mills theory and in the string theory dual
The near horizon geometry of the D3-D5 system contains two sets of excitations, those of closed IIB superstrings occupying AdS5, which are dual to N = 4 supersymmetric Yang-Mills theory on the R4 boundary of AdS5, and open strings connecting the D3 and D5 branes, which are dual to field theory excitations on the R3 boundary of AdS4, the latter forming a co-dimension one defect in R4
Summary
Probe branes and defect conformal field theories have been widely studied in the context of AdS/CFT holography [1]-[23]. In an interesting recent paper [25], Nagasaki and Yamaguchi showed that the one-point functions of chiral primary operators could be computed for the D3-D5 defect field theory in the limit of large monopole number k. The situation on the gauge theory side is again as illustrated, only in the first case the parameter k gets replaced by k1k2 and in the second case it gets replaced by dG Even in these non-supersymmetric systems, the one-point functions of chiral primary operators on the string and gauge theory sides agree in the leading order of a large , √k1 √k2 limit of the SO(3) × SO(3) symmetric λλ system, O∆(x) = k√1k2 ∆.
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