AdS/CFT and QCD

TL;DR

This paper explores how the AdS/CFT correspondence provides a semi-classical, analytic model for strongly-coupled QCD, linking higher-dimensional theories to hadron structure and non-perturbative phenomena.

Contribution

It establishes a precise connection between AdS space variables and hadron constituents, deriving analytic light-front wavefunctions and new relativistic equations for QCD.

Findings

Exact correspondence between AdS coordinate z and impact variable zeta.

Derivation of analytic, frame-independent light-front wavefunctions.

Introduction of new relativistic light-front equations with algebraic structures.

Abstract

The AdS/CFT correspondence between string theory in AdS space and conformal field theories in physical space-time leads to an analytic, semi-classical model for strongly-coupled QCD which has scale invariance and dimensional counting at short distances and color confinement at large distances. Although QCD is not conformally invariant, one can nevertheless use the mathematical representation of the conformal group in five-dimensional anti-de Sitter space to construct a first approximation to the theory. The AdS/CFT correspondence also provides insights into the inherently non-perturbative aspects of QCD, such as the orbital and radial spectra of hadrons and the form of hadronic wavefunctions. In particular, we show that there is an exact correspondence between the fifth-dimensional coordinate of AdS space z and a specific impact variable zeta which measures the separation of the quark and gluonic constituents within the hadron in ordinary space-time. This connection allows one to compute the analytic form of the frame-independent light-front wavefunctions, the fundamental entities which encode hadron properties and allow the computation of decay constants, form factors, and other exclusive scattering amplitudes. New relativistic light-front equations in ordinary space-time are found which reproduce the results obtained using the 5-dimensional theory. The effective light-front equations possess remarkable algebraic structures and integrability properties. Since they are complete and orthonormal, the AdS/CFT model wavefunctions can also be used as a basis for the diagonalization of the full light-front QCD Hamiltonian, thus systematically improving the AdS/CFT approximation.