Abstract. The interface of neutral Rydberg atoms in the gas phase with a solid surface is of interest in many fields of modern research. This interface poses a particular challenge for any application in which Rydberg atoms are close to a substrate but also opens up the possibility of studying properties of the surface material itself through the atomic response. In this review the focus is on the process of electron tunneling from the excited state into the substrate that occurs when a Rydberg atom is located in front of a surface at a range of a few hundred nm and is demonstrated with a metallic surface. It is shown how variations in this ionisation mechanism can provide a powerful tool to probe imagecharge effects, measure small superficial electric stray or patch fields and how charge transfer from the Rydberg atom can be in resonance with energetically discrete surface states.
Rydberg atoms at surfaces and interfacesWhen atoms are excited into states of high principal quantum number n their properties are exaggerated and long-range interactions lead to a strong coupling with their environment. The electron cloud is greatly expanded compared to the ground state (∝ n 2 ) which results in a large polarisability of a Rydberg state (∝ n 7 ) causing a strong response to electric fields [1]. In terms of a classical dipole, the positive core and negative electron are widely separated giving these excited states a large dipole moment, by which Rydberg atoms exhibit interactions over great distances (∼ μm), where the interactions can be controlled externally. The range of exotic properties makes them an interesting subject in various fields of research, Rydberg atoms are used in cavity quantum electrodynamics [2,3], in controlled chemical reactions by mechanical manipulation [4], serve as a model system for dipole-mediated energy transport in biological systems [5], can be used as a non-linear medium to mediate single-photon interactions [6,7] and have been proposed in several ways for quantum information processing [9][10][11][12]. However, this also means that the strong interaction will not be limited to surrounding atoms but that they also couple to condensed matter, bulk surfaces, in the vicinity. See Fig. 1 for an overview of Rydberg-surface interactions.a