We investigate the Quantum-Electro-Dynamic properties of an atomic electron close to the focus of a spherical mirror. We first show that the spontaneous emission and excited state level shift of the atom can be fully suppressed with mirror-atom distances of many wavelengths. A three-dimensional theory predicts that the spectral density of vacuum fluctuations can indeed vanish within a volume λ 3 around the atom, with the use of a far distant mirror covering only half of the atomic emission solid angle. The modification of these QED atomic properties is also computed as a function of the mirror size and large effects are found for only moderate numerical apertures. We also evaluate the long distance ground state energy shift (Casimir-Polder shift) and find that it scales as (λ/R) 2 at the focus of a hemi-spherical mirror of radius R, as opposed to the well known (λ/R) 4 scaling law for an atom at a distance R from an infinite plane mirror. Our results are relevant for investigations of QED effects, and also free space coupling to single atoms using high-numerical aperture lenses.PACS numbers: 42.25.-p, 12.20.-m, 37.30.+i Spontaneous emission and level shifts of atoms can be notably altered by placing them between mirrors. By modifying the electromagnetic mode structure interacting with the atomic electron [1], one obtains a significant change in these quantum-electrodynamic (QED) atomic properties. Most experimental studies make use of high finesse cavities [2][3][4][5][6][7] to see the effects. Another way to change the properties of single emitters is to place other identical atoms close-by as originally propounded by Dicke [8]. To observe large QED effects in this case, the dipole emission patterns have to overlap, which requires the atoms to be very close to each other. Such effects were analyzed using two trapped ions [9], but the Coulomb interaction between the ions restricted their distance to a few microns. The interaction between two neutral atoms is however not overwhelmed by the Coulomb force. Using the large dipole moments of nearby Rydberg atoms localised in a dipole trap, entanglement between neutral atoms was recently demonstrated [10,11].In general, an atom close to a single mirror already provides a very efficient way to investigate QED effects. The resonance fluorescence of a Doppler cooled Barium ion was reflected back onto itself in [12], using a large numerical aperture (NA) lens and a mirror that was 30 cm away from the ion. In this experiment, the description of the interaction between the atom and the modified electromagnetic field, or the mirror image, is very similar to the direct dipole-dipole coupling between two real atoms. Here, due to the high numerical aperture of the collection lens, the mode structure was altered significantly even if the mirror was many wavelengths away from the ion. A 1% change in the decay rate was measured and found to be mostly limited by the collection solid angle and residual atomic motion. Such a system also leads to a vacuum-induced level shift in a l...