Abstract
Positron lifetimes in polybutadiene (PB) and polypropylene (PP) are measured as functions of temperature in the range 95–305 K and 95–370 K, respectively. From the variations of ortho-positronium (o-Ps) lifetime τ3, we have determined the glass transition temperatures Tg in PB and PP and the excluding temperature Te in PB, beyond which the o-Ps lifetime τ3 in PB is saturated. From the analogy of the temperature-dependent o-Ps intensity I3 in PB and PP, high- and low-density polyethylene (HDPE and LDPE), we propose that above the glass transition temperature Tg the o-Ps intensity I3 exhibits the scaling relation I3∼(T-Tg )β in these polymers. The data also indicate the existence of a crossover temperature Tc, located above Tg, where the β value changes greatly. When TgT≤Tc, β has the order of magnitude of 102. When TcTTe, β=0.346±0.035 and 0.297±0.037 for linear polymers PB and PP. Similar features are also observed for previous results of HDPE and LDPE [D. Lin and S. J. Wang, J. Phys. Condens. Matter 4, 3331 (1992)]. The β values in the region of TcTTe are found to be 0.336±0.038 and 0.507±0.059 for linear polymers HDPE and branched LDPE, respectively. These results reveal a common picture of hole creation above Tg in polymers, however, the concrete value of β may be associated with the branching structure of macromolecules.