We report the first experimental observation of negatively charged hydrogen and deuterium cluster ions, H − n and D − n , where n ≥ 5. These anions are formed by an electron addition to liquid helium nanodroplets doped with molecular hydrogen or deuterium. The ions are stable for at least the lifetime of the experiment, which is several tens of microseconds. Only anions with odd values of n are detected, and some specific ions show anomalously high abundances. The sizes of these "magic number" ions suggest an icosahedral framework of H 2 (D 2 ) molecules in solvent shells around a central H − (D − ) ion. The first three shells, which contain a total of 44 H 2 or D 2 molecules, appear to be solidlike, but thereafter a more liquidlike arrangement of the H 2 (D 2 ) molecules is adopted. to be strongly bent rather than linear. Consequently, there are real doubts about the basic structures of H − n ions that need to be resolved, and given that there are no reliable estimates of the actual dissociation energies (D 0 ) of these clusters, it is not even clear if anions with n > 3 are stable.Here we report the first experimental detection of anionic hydrogen and deuterium clusters larger than H − 3 =D − 3 and have done so for a wide range of cluster sizes. The experimental procedure involved the formation of the corresponding neutral ðH 2 Þ N and ðD 2 Þ N clusters by adding H 2 or D 2 gas to liquid helium nanodroplets. The neutral clusters were cooled to the ambient temperature of the helium nanodroplets, 0.38 K [13], prior to an impact by a beam of electrons with a controlled energy. H 2 and D 2 are heliophilic (have a negative chemical potential when immersed in liquid helium [13]) and so will reside inside the helium droplets rather than on the surface. The helium droplets were then exposed to a beam of electrons, which generated anionic products in the gas phase that were detected by mass spectrometry. The transfer of negative charge to the ðH 2 Þ n and ðD 2 Þ N clusters occurs via a mobile electron bubble, whose formation has a threshold energy in excess of 1 eV in order to inject the electron into the helium conduction band [14]. The droplets used in the present work were relatively large (∼10 6 helium atoms), and for droplets of this size the electron bubble, although