Polymer Institute of SAS, Dúbravská cesta 9, SK-845 41 Bratislava, Slovak Republic.
J Phys Condens Matter. 2012 Apr 18;24(15):155104. doi: 10.1088/0953-8984/24/15/155104. Epub 2012 Mar 22.
We report on the temperature dependence of the lifetime of the ortho-positronium (o-Ps), τ(3), annihilation in amorphous polymer poly(vinylmethylether) (PVME) from positron annihilation lifetime spectroscopy (PALS). We show that the behavior of τ(3)(T) can be divided into five regions, each of them having a linear temperature dependence, and that the crossover PALS temperatures situated at T(b1)(G), 0.76T(g)(PALS), T(b1)(L) = 1.14T(g)(PALS) and T(b2)(L) = 1.37T(G)(PALS), and marking the discontinuity in the free volume microstructure are related to various dynamic features from neutron scattering (NS) and broadband dielectric spectroscopy (BDS). First, a slight change in the PALS response in the glassy PVME at T(b1)(G) is related to the onset of the excess wing in an apparent correspondence with the fast secondary β motion from NS. A further slight bend in the liquid state at T(b1)(L) is related to a high-frequency tail of the primary α process as well as to the slow secondary β relaxation from BDS. In addition, it lies also in the vicinity of the crossover temperature, T(B)(βKWW), in the spectral dispersion of the primary α process, indicating a connection of the change in the o-Ps lifetime with the variation in the width of the primary α relaxation times distribution. Finally, the τ(3) value at T(b2)(L) is close to the mean relaxation time of the primary α process, τ(α), in coincidence with the crossover in the secondary effective β process between two regimes in the liquid PVME. All these relationships point to very close connections between the PALS response and the dynamic behavior of PVME, which can be explained in terms of the temperature dependence of the probability function of the liquid-like and the solid-like domains, as obtained from the two-order parameter (TOP) model description of the liquid to glass transition in glass-formers.
我们报告了在非晶态聚合物聚(甲基乙烯基醚)(PVME)中,正电子素(o-Ps)的寿命τ(3)的湮灭的温度依赖性,这是通过正电子湮没寿命谱(PALS)得到的。我们表明,τ(3)(T)的行为可以分为五个区域,每个区域都具有线性温度依赖性,并且 PALS 温度交叉点 T(b1)(G)、0.76T(g)(PALS)、T(b1)(L)=1.14T(g)(PALS)和 T(b2)(L)=1.37T(G)(PALS)与来自中子散射(NS)和宽带介电谱(BDS)的各种动态特征有关。首先,在玻璃态 PVME 中 PALS 响应的轻微变化与在 NS 中观察到的快速次级β运动的附加翼的开始有关。在液体状态下,进一步的轻微弯曲在 T(b1)(L)处与初级α过程的高频尾部以及 BDS 中的缓慢次级β松弛有关。此外,它也位于初级α过程的谱色散中交叉温度 T(B)(βKWW)附近,表明 o-Ps 寿命的变化与初级α松弛时间分布的宽度变化有关。最后,在 T(b2)(L)处的τ(3)值接近初级α过程的平均松弛时间τ(α),与液体 PVME 中两个区域之间的次级有效β过程的交叉相吻合。所有这些关系都表明 PALS 响应与 PVME 的动态行为之间存在非常密切的联系,可以根据液体到玻璃转变的两参数(TOP)模型描述,从液体和固体状态的概率函数的温度依赖性来解释。