Since the discovery of the hydrated electron more than 40 years ago, a general consensus has emerged that the hydrated electron occupies a quasispherical cavity in liquid water. We simulated the electronic structure and dynamics of the hydrated electron using a rigorously derived pseudopotential to treat the electron-water interaction, which incorporates attractive oxygen and repulsive hydrogen features that have not been included in previous pseudopotentials. What emerged was a hydrated electron that did not reside in a cavity but instead occupied a~1-nanometer-diameter region of enhanced water density. Both the calculated ground-state absorption spectrum and the excited-state spectral dynamics after simulated photoexcitation of this noncavity hydrated electron showed excellent agreement with experiment. The relaxation pathway involves a rapid internal conversion followed by slow ground-state cooling, the opposite of the mechanism implicated by simulations in which the hydrated electron occupies a cavity.T he nature of excess electrons in liquid water has been of continuing interest due to their important role in radiation chemistry and charge-transfer reactions. Excess electrons can be created directly by pulse radiolysis, or they can be formed after ionization of a solute if the detached electron resides in the liquid far from its parent cation. When liquid water locally contains one more electron than is needed to maintain electrical neutrality, the metastable localized species that is created has been termed the hydrated electron ( e − aq ). The hydrated electron has attracted considerable theoretical interest, in part because it poses the intriguing question of how a polar solvent acts to localize an object whose size and shape is determined self-consistently by interaction with its surroundings. Thus, although the hydrated electron is nominally a simple singleelectron species, the many-body nature of its interactions with the surrounding water molecules has made this a nontrivial problem in statistical mechanics and quantum chemistry that can directly confront experiment.Early continuum and semicontinuum models treated the hydrated electron as a spherical charge distribution with a radius determined selfconsistently by polarization of the surrounding solvent. Such models provided insight into the mechanism by which electrons may be localized but did not give a microscopic picture for the structure of the solvent in the presence of the e − aq . Subsequent studies used molecular simulations to address such structural questions; in such simulations, the excess electron was treated quantum-mechanically, the surrounding water molecules were treated classically, and the electronwater interaction was described by what is known formally as a pseudopotential (1-3). Although alternatives have been proposed (4), the consensus picture that emerged from such simulations was that a hydrated electron excludes water from a small region, so that the e − aq occupies a nearly spherical void that is surrounded by water molec...