A series of hyperbranched polylactides (HB-PLLAs) with different branching densities were prepared by the selfpolycondensation of AB 2 -type macromonomers (degree of polymerization of polylactides (n) = 5. 0, 8.4, 19, 29, and 42). The high-molecular-weight HB-PLLAs (M w = 4.95 × 10 4 −1.47 × 10 5 ) were prepared in good yields. Molecular characterizations of the HB-PLLAs were meticulously performed by size-exclusion chromatography at 25 °C using a system equipped with multiangle laser light scattering (SEC-MALS) and 1,1,1,3,3,3-hexafluoro-2-propanol (HFIP) as the eluent. The z-averaged root-mean-square radius of gyrations (⟨S 2 ⟩ z 1/2 ) of the HB-PLLAs in HFIP at 25 °C were much smaller than those of the linear PLLA with the corresponding weight-average molecular weight (M w ), supporting the presence of the branched architectures. The M w dependence of ⟨S 2 ⟩ z 1/2 of the HB-PLLAs was determined to follow the equations ⟨S 2 ⟩ z 1/2 (nm) = 2.5 × 10 −1 M w 0.37 for n = 8.4, ⟨S 2 ⟩ z 1/2 (nm) = 1.8 × 10 −1 M w 0.40 for n = 19, ⟨S 2 ⟩ z 1/2 (nm) = 1.6 × 10 −1 M w 0.41 for n = 29, and ⟨S 2 ⟩ z 1/2 (nm) = 1.1 × 10 −1 M w 0.44 for n = 42 in HFIP at 25 °C. A comparison of the experimental and theoretical results with respect to their dimensional properties indicated that the HB-PLLAs assume randomly branched architectures (i.e., a hyperbranched structure). The DSC and X-ray diffraction measurements suggested that the crystallization was remarkably suppressed by the introduction of the branched architecture.