Secondary electrons with low energy (< 10 eV) are produced in large quantities along the ionization pathway when highenergy quanta interact with biological material.[1] These electrons are able to induce strand breaks in plasmid DNA [2] at energies near 0 eV. [3,4] The underlying molecular mechanisms are still under debate, but it is well established that dissociative electron attachment (DEA) plays a pivotal role. [5,6] The single building blocks of DNA (nucleobases, sugars, and phosphates) have been well studied. [5,[7][8][9] To obtain information on the molecular mechanisms of strand breaks, however, it is crucial to know how a negative charge evolves in a biomolecular system that is composed of more than one subunit of DNA. For example, it was proposed from a theoretical study that an initial capture of an electron by a nucleobase and subsequent transfer of the negative charge to the DNA backbone results in cleavage of a phosphate-sugar bond. [10][11][12][13] A competing pathway is direct DEA to the phosphate group [9,14] or to the sugar unit. [8,15] The experimental investigation of relevant molecular systems such as nucleosides, sugar phosphates, and nucleotides is particularly challenging since they are thermally labile and nonvolatile. To overcome the experimental shortcomings and to enable a completely new range of experiments we applied laserinduced acoustic desorption (LIAD) [16] of neutral biomolecules to study dissociative electron attachment in the gas phase. Here we present results on DEA to the nucleoside thymidine (Td) and to d-ribose-5-phosphate (RP), the latter serves as a model compound for the DNA or RNA backbone. We present the first experimental evidence that electrons with energies close to 0 eV are resonantly captured by RP in the gas phase with subsequent cleavage of the sugar-phosphate linkage.It was shown previously that LIAD is suitable for transfering neutral intact biomolecules into the gas phase. [16,17] A detailed description of the currently used apparatus is given elsewhere.[18] In brief, a solution of sample molecules in methanol is deposited on a thin titanium foil (12.7 mm, Alfa Aesar), and the solvent quickly removed at low pressure to form a uniform layer. The coated titanium foil is then introduced into a high vacuum chamber and irradiated from the reverse side with a pulsed Nd:YAG laser (532 nm, 3 mJ pulse À1 , repetition rate 15 Hz). The short laser pulse (2-6 ns) generates a shock wave that propagates through the metal to the opposite surface, ultimately leading exclusively to a gentle desorption of neutral and intact molecules. The desorbed molecules then interact with an electron beam of defined energy, and the generated anions are then analyzed by means of a quadrupole mass spectrometer. The sample holder is moveable in one direction so that the irradiated spot can be moved along the entire foil.The electron beam is generated by a simple electron gun composed of a tungsten filament and four molybdenum electrodes. The electrons are guided along a homogeneous magnetic ...