The nanobubble inflation method is the only experimental technique that can measure the viscoelastic creep compliance of unsupported ultrathin films of polymers over the glass-rubber transition zone as well as the dependence of the glass transition temperature (T g ) on film thickness. Sizeable reduction of T g was observed in polystyrene (PS) and bisphenol A polycarbonate by the shift of the creep compliance to shorter times. The dependence of T g on film thickness is consistent with the published data of free-standing PS ultrathin films. However, accompanying the shift of the compliance to shorter times, a decrease in the rubbery plateau compliance is observed. The decrease becomes more dramatic in thinner films and at lower temperatures. This anomalous viscoelastic behavior was also observed in poly(vinyl acetate) and poly (n-butyl methacrylate), but with large variation in the change of either the T g or the plateau compliance. By now, well established in bulk polymers is the presence of three different viscoelastic mechanisms in the glass-rubber transition zone, namely, the Rouse modes, the sub-Rouse modes, and the segmental a-relaxation. Based on the thermorheological complexity of the three mechanisms, the viscoelastic anomaly observed in ultrathin polymer films and its dependence on chemical structure are explained in the framework of the Coupling Model.Next, the softening dispersion of PBMA had been obtained by the measurements of the complex shear compliance (J* ¼ J 0 À J 00 ) in the frequency range from 24 to 2400 cycles by Child and Ferry. 79 Both J 0 and J 00 show very broad width of