Fig. 1: Temperature dependence of the atomic dynamics in Pt42.5Cu27Ni9.5P21 and Pd42.5Cu27Ni9.5P21 supercooled liquids. | Communications Physics

Fig. 1: Temperature dependence of the atomic dynamics in Pt42.5Cu27Ni9.5P21 and Pd42.5Cu27Ni9.5P21 supercooled liquids.

From: Disentangling structural and kinetic components of the α-relaxation in supercooled metallic liquids

Fig. 1

a, b Normalized intensity autocorrelation functions measured at various temperatures for Pt42.5Cu27Ni9.5P21 (a), and Pd42.5Cu27Ni9.5P21 (b) at the wave vector Q of the first sharp diffraction peak (QFSDP ≈ 2.8 Å−1 for both systems). c, d Mean relaxation time <τ(Q,T)> of the Pt- and Pd-based alloys measured at the position of the first sharp diffraction peak QFSDP at various temperatures T. The solid lines are fits to the Vogel-Fulcher-Tammann equation (see section “Collective particle motion in the supercooled liquid phase”). e, f Temperature dependence of the corresponding exponent of the Kohlrausch-William-Watts equation β(Q,T) for Pt42.5Cu27Ni9.5P21 (e) and Pd42.5Cu27Ni9.5P21 (f). The dashed line is a guide to the eyes. Error bars indicate the standard error due to fitting of the experimental data using the Levenberg Marquardt algorithm.

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