Electrical resistivity, specific heat, and magnetization measurements to temperatures as low as 80 mK and magnetic fields up to 16 T were made on the filled skutterudite compound PrOs4As12. The measurements reveal the presence of two ordered phases at temperatures below approximately 2.3 K and in fields below approximately 3 T. Neutron-scattering experiments in zero field establish an antiferromagnetic ground state <2.28 K. In the antiferromagnetically ordered state, the electronic-specific heat coefficient ␥ Ϸ 1 J͞mol⅐K 2 below 1.6 K and 0 < H < 1.25 T. The temperature and magnetic-field dependence of the electrical resistivity and specific heat in the paramagnetic state are consistent with single-ion Kondo behavior with a low Kondo temperature on the order of 1 K. The electronic-specific heat in the paramagnetic state can be described by the resonance-level model with a large zero-temperature electronic-specific heat coefficient that decreases with increasing magnetic field from approximately 1 J͞mol⅐K 2 at 3 T to approximately 0.2 J͞mol⅐K 2 at 16 T.heavy fermion ͉ Kondo effect ͉ antiferromagnetism T he compound PrOs 4 As 12 belongs to the family of filled skutterudites, which have the formula AT 4 X 12 , where A ϭ alkali metal, alkaline earth, lanthanide, or actinide, T ϭ Fe, Os, or Ir, and X ϭ P, As, or Sb. Because the ions reside in an atomic cage with a large number of X nearest neighbors, the hybridization between the lanthanide filler ion localized 4f states and the conduction-electron states is appreciable, often resulting in strongly correlated electron phenomena. In a recent article (1), we reported a study of the physical properties of single crystals of the filled skutterudite compound PrOs 4 As 12 between approximately 0.4 and 300 K by means of magnetization M, specific heat C, and electrical resistivity measurements. The previous study revealed that the compound exhibits two (possibly three) ordered phases below approximately 2.5 K in zero field and approximately 3 T at zero temperature from kinks in M as a function of magnetic field H and temperature T. Features in the (T) and C(T) data in zero field can be identified with transitions into the two ordered phases below 2.5 K. The magnetic susceptibility conforms to a Curie-Weiss law below approximately 20 K with an effective magnetic moment eff ϭ 2.77 B ͞formula unit consistent with a ⌫ 5 ground state in a cubic crystalline electric field and a cusp at approximately 2.5 K, indicative of antiferromagnetic (AFM) order. These results provide another example of the wide range of correlated electron ground states that are found in the Pr-based filled skutterudites, which include conventional (Bardeen, Cooper, Schrieffer) superconductivity (e.g., PrRu 4 Sb 12 ) (2), unconventional superconductivity (e.g., PrOs 4 Sb 12 ) (3, 4), heavy fermion behavior (e.g., PrFe 4 P 12 , PrOs 4 Sb 12 ) (5-8), antiferroquadrupolar order (e.g., PrFe 4 P 12 , PrOs 4 Sb 12 ), and magnetic order (e.g., PrFe 4 Sb 12 ) (9, 10). In this article, we report measurements of the te...