When UV light ionises water, hydrated electrons are produced. [1] Radiation damage of DNA and RNA is thought to originate from attachment of these electrons to nucleobases.[2] The formed radical anions participate in chemical reactions that lead to alterations in their original structure and to loss of genetic information. Hence, the interaction between electrons and DNA and RNA is a field of intense research with the goal of understanding the biological damage by the ™free∫ electrons. DNA and RNA are composed of nucleotides which consist of a nucleobase, a furanose sugar, and a phosphate group. A reductionist approach has been taken in the study of electron attachment to isolated nucleobases in vacuum to elucidate the electronic structure of the anion and to show how Watson ± Crick base-pairing is affected, if at all.[3±15] It is well-documented that electron affinities (EAs) are positive due to the existence of dipole-bound states. [6,7] The dipole moment of adenine just suffices to support such a state whereas occupation of the LUMO (lowest unoccupied molecular orbital) to form a covalent anion is energetically unfavourable. [5,6,9] Here, we move one step further and describe electron binding to nucleotides, the intact building blocks, based on a combination of experiments and theoretical calculations.A nucleotide carries a negative charge located on the phosphate group. Direct attachment of low kinetic energy electrons (% 0 eV) to anions in vacuum is hindered by a large Coulomb barrier and is only possible through tunnelling. To circumvent this hindrance we have collided nucleotide monoanions which have high translational kinetic energy (50 keV) with gaseous sodium and looked for electron capture. The idea was that an electron jump might happen at close approach beyond the Coulomb barrier, an electron might ™sneak in∫ when attached to a sodium atom. In this way we try to mimic the actual situation in solution phase where the Coulomb barrier is less important.The mass-analyzed ion kinetic energy (MIKE) spectrum obtained for the collision between the AMP anion (adenosine 5'-monophosphate, m/z 346, Scheme 1) and sodium is shown in Figure 1 B. A spectrum for collisions with neon is included for comparison (Figure 1 A). The geometrical cross section of neon is similar to that of sodium but neon's much larger ionization energy prevents electron transfer. Peaks corresponding to fragment ions are seen in both spectra. Interestingly, however, a peak at half the m/z value of the parent ion appears when sodium is used as the collision gas but is absent when neon is used. In dissociation processes kinetic energy is released with the result of broad peaks in the MIKE spectra. The peak width of the ion at half the m/z is narrower than that of other peaks, which implies that this ion is not a fragment ion but instead a dianion. The accuracy of the calibration is not adequate to determine whether the doubly charged ion is the AMP dianion or the AMP dianion minus a hydrogen atom, but B3LYP6 ± 311 G(2d,p)//PM3 calculations...