Solvable Relativistic Hydrogenlike System in Supersymmetric Yang-Mills Theory
arXiv:1408.0296 · doi:10.1103/PhysRevLett.113.161601
Abstract
The classical Kepler problem, as well as its quantum mechanical version, the Hydrogen atom, enjoy a well-known hidden symmetry, the conservation of the Laplace-Runge-Lenz vector, which makes these problems superintegrable. Is there a relativistic quantum field theory extension that preserves this symmetry? In this Letter we show that the answer is positive: in the non-relativistic limit, we identify the dual conformal symmetry of planar super Yang-Mills with the well-known symmetries of the Hydrogen atom. We point out that the dual conformal symmetry offers a novel way to compute the spectrum of bound states of massive bosons in the theory. We perform nontrivial tests of this setup at weak and strong coupling, and comment on the possible extension to arbitrary values of the coupling.
4 pages, 3 figures. Clarifications added; published version
References in corpus (6)
- Gluon scattering amplitudes at strong coupling
- Iterative structure of finite loop integrals
- Higgs-regularized three-loop four-gluon amplitude in N=4 SYM: exponentiation and Regge limits
- Spinor Helicity and Dual Conformal Symmetry in Ten Dimensions
- Dual Conformal Properties of Six-Dimensional Maximal Super Yang-Mills Amplitudes
- The static potential in {\cal N}=4 supersymmetric Yang-Mills at weak coupling
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