Notes on D-instanton correction to $AdS_5 \times S^5$ geometry

TL;DR

This paper explores the geometric and physical implications of D-instantons in $AdS_5 imes S^5$, revealing their wormhole nature, symmetry constraints, and effects on string coupling and background geometry.

Contribution

It demonstrates that D-instantons act as wormholes connecting $AdS_5 imes S^5$ to flat space and analyzes the impact of $SL(2,{f R})$ symmetry on the background and coupling.

Findings

D-instantons are wormholes linking $AdS_5 imes S^5$ to flat space.

No $SL(2,{f R})$ transformation can weaken the string coupling without affecting the axion.

Discussion of D-instanton effects in $AdS_3$ and instanton gases.

Abstract

We show that the D-instanton in the $AdS_5 \times S^5$ background is a wormhole connecting the background $AdS_5 \times S^5$ to the flat space $\bf R^{10}$ located at the position of the D-instanton. By a $SL(2,{\bf R})$ rotation of type IIB theory, we can make the {\it global} geometry flat in string frame. We also find that, due to the tight relation between the dilaton and the axion, there is no $SL(2,{\bf R})$ element that takes strong string coupling to weak one without making the axion ill defined. We also discuss the case of $AdS_3$ as well as the instanton gases. A subtlety on the D-instanton at the boundary or at the horizon is discussed.