We combine measurements of the longitudinal (Ï xx ) and Hall (Ï xy ) resistivities of disordered 2D amorphous indium-oxide films to study the magnetic-field tuned superconductor-to-insulator transition (H-SIT) in the T â 0 limit. At the critical field, H c , the full resistivity tensor is T independent with Ï xx (H c ) = h/ 4e 2 and Ï xy (H c ) = 0 within experimental uncertainty in all films (i.e., these appear to be "universal" values); this is strongly suggestive that there is a particlevortex self-duality at H = H c . The transition separates the (presumably) superconducting state at H < H c from a "Hall-insulator" phase in which Ï xx â â as T â 0 whereas Ï xy approaches a nonzero value smaller than its "classical value" H/ nec; i.e., 0 < Ï xy < H/ nec. A still higher characteristic magnetic field, H c * > H c , at which the Hall resistance is T independent and roughly equal to its classical value, Ï xy â H/ nec, marks an additional crossover to a high-field regime (probably to a Fermi insulator) in which Ï xy > H/ nec and possibly diverges as T â 0. We also highlight a profound analogy between the H-SIT and quantum-Hall liquid-to-insulator transitions (QHIT).superconductor-insulator transition | quantum phase transition | self-duality | Hall insulator Q uantum phase transitions (QPTs) occur at zero temperature (T = 0) as a quantum control parameter is varied. Where the transition is continuous, quantum critical phenomena are expected to give rise to universal physics that can be analyzed using a straightforward scaling theory. The magnetic-field tuned transition between superconducting and insulating ground states in 2D conductors is a particularly attractive exemplar of a QPT because the magnetic field can be continuously tuned, allowing a detailed scaling analysis of the QPTs and explorations of the ground-state phases proximate to criticality (1-9). However, the exact nature of the insulating and superconducting states above and below the magnetic-field tuned superconductor-to-insulator transition (H-SIT) and a satisfactory description of the transition between them are still lacking.The conventional picture of T â 0 phases of a 2D electron fluid in the presence of disorder is based on the assumption that the only stable phases are superconducting or insulating (or, in a magnetic field, quantum Hall liquid phases). In contrast, studies of films near the H-SIT have suggested the existence of several unexpected new ground-state phases in films that superconduct at zero field. In weakly disordered films (with normal state resistivity small compared with the quantum of resistance, Ï N h=e 2 ), the superconducting state gives way to an "anomalous metallic phase" with a resistivity that extrapolates to a nonzero value, 0 < ÏĂ°T â 0, HĂ Ï N