Positronium (Ps) is widely used as a probe for studying nanometric porosities in condensed matter. Accessible experimental measurements concern annihilation rates by pickoff processes and contact densities (the electron density at the positron position). Existing models for describing Ps properties in small cavities do not justify the lowering of the contact density with respect to that of Ps in vacuum, as found in most materials. We formulate a two-particle model in which only the electron is confined in the cavity, while the positron is moving freely and feels the medium via a positive work function. Our calculation fully explains experimental data for a large class of materials and suggests a way to gain information on pore sizes and positron work functions. DOI: 10.1103/PhysRevLett.116.033401 Positronium (Ps) is a hydrogenlike bound state of an electron and its antiparticle, the positron. Ps can exist in two different states: the singlet state p-Ps, rapidly decaying into 2γ rays with a lifetime of 0.125 ns, and the triplet state o-Ps annihilating in 3γ rays with a lifetime of 142 ns in vacuum [1]. Ps is usually formed by implanting positrons in condensed matter. Many insulators and molecular solids allow Ps formation, sometimes with high efficiency; when generated near the surface (e.g., by using a slow positron beam) Ps can rapidly spread toward the surface and eventually be released into the vacuum [2]. In porous materials, o-Ps is also emitted into cavities, and, mainly in subnanometricsized voids, its lifetime can be notably reduced by pickoff annihilation: the o-Ps positron can annihilate via 2γ decay with an electron of the surrounding cavity walls if a relative singlet state is realized [3]. This property is at the heart of the use of Ps as a probe for studying nanoscale structures in condensed matter. In fact, while 2γ annihilation in vacuum depends on the electron density at the positron position (the contact density [4]), pickoff processes depend on the electron density in the bulk around the cavity.Experimental data obtained with the positron annihilation lifetime spectroscopy technique, also in the presence of a magnetic field (via magnetic quenching), primarily concern pickoff annihilation with lifetimes as low as a few ns [5,6]. The contact density can be determined from fitting lifetime spectra [7]. In molecular solids, this quantity is usually found to be well below the vacuum value. It is of paramount importance to connect these measurable quantities with the properties of Ps in small cavities as a means to obtain information on pore dimensions and other material characteristics.To describe Ps inside small cavities, the most used models are based on the Tao-Eldrup approach [8][9][10][11], which relates pickoff annihilation rates to pore sizes by considering Ps as a single quantum particle. Consequently, these models cannot give information about contact density and are suitable only when cavities are much larger than twice the Ps Bohr radius α 0 ¼ 0.106 nm. Another family of models, more ...