The present paper illustrates key features of charge transfer between calcium atoms and prototype conjugated hydrocarbons (ethylene, benzene, and coronene) as elucidated by electronic structure calculations. One-and two-electron charge transfer is controlled by two sequential conical intersections. The two lowest electronic states that undergo a conical intersection have closedshell and open-shell dominant configurations correlating with the 4s 2 and 4s 1 3d 1 states of Ca, respectively. Unlike the neutralionic state crossing in, for example, hydrogen halides or alkali halides, the path from separated reactants to the conical intersection region is uphill and the charge-transferred state is a biradical. The lowest-energy adiabatic singlet state shows at least two minima along a single approach path of Ca to the π system: (i) a van der Waals complex with a doubly occupied highest molecular orbital, denoted ϕ 2 1 , and a small negative charge on Ca and (ii) an open-shell singlet (biradical) at intermediate approach (Ca⋯C distance ≈2.5-2.7 Å) with molecular orbital structure ϕ 1 ϕ 2 , where ϕ 2 is an orbital showing significant charge transfer form Ca to the π-system, leading to a one-electron multicentered bond. A third minimum (iii) at shorter distances along the same path corresponding to a closed-shell state with molecular orbital structure ϕ 2 2 has also been found; however, it does not necessarily represent the ground state at a given Ca⋯C distance in all three systems. The topography of the lowest adiabatic singlet potential energy surface is due to the one-and two-electron bonding patterns in Ca-π complexes.metal atom | metastable state | nature of metal-π binding | one-and two-electron multicentered bonds | triplet ground state T he interactions of metal atoms with alkenes, polyenes, aromatics, and graphene-based materials are important for applications in catalysis (1, 2), molecular electronics (3-6), optoelectronic and sensing devices (7,8), and hydrogen storage materials (9-12). Charge transfer from the metal to the organic system is one of the key features determining adsorption energies, reactivities, electronic structure, conductivities, and optical properties (4,8). Most studies of charge transfer have focused on equilibrium geometries (4, 13-15), but the design of molecular devices and the understanding of adsorption and reactivity also require understanding the dependence of charge transfer on molecular geometry (16). In this communication we show that charge transfer character can change rapidly and suddenly for small changes in geometry, and we explain this phenomenon in terms of conical intersections (CIs). In addition we show that the charge transfer state can be a ferromagnetically coupled biradical, which is relevant to the possibility of control of magnetization by an electric field in, for example, spintronics applications (17). A fundamental understanding of the interfacial states of metal atoms interacting with conjugated π-systems is an essential element underlying rational molecular el...