content_image/408461.jpg content_image/408463.jpg content_image/408462.jpg content_image/408464.jpg
<img src='content_image/408461.jpg'>

<img src='content_image/408463.jpg'>

and symbol shape indicates the final temperature T$_{f}$ . 

We find that t Cq r ( t$_{w}$ ) is characterized by three differ- ent t$_{w}$ -windows. (I) For waiting times t$_{w}$ ≲ 0 . 3 ns, de- cay times are significantly lower for T$_{i}$ = 5000 K (black lines and symbols) than for T$_{i}$ = 3760 K (green/gray lines and symbols). The dependence of t Cq r on t$_{w}$ is strongly dependent on all varied parameters, i.e. T$_{i}$ , T$_{f}$ , particle type, and q . For T$_{i}$ = 5000 K, T$_{f}$ = 2500 K, 2750 K, and 

<img src='content_image/408462.jpg'>

<img src='content_image/408464.jpg'>

q = 1 . 7 ˚ A − $^{1}$, 2 . 7 ˚ A − 1 t Cq r ( t$_{w}$ ) follows roughly a power law with an exponent µ ≈ 1 . 15 with variations of the order of 0 . 07 dependent on T$_{f}$ , particle type, and q . (II) For intermediate waiting times, t Cq r ( t$_{w}$ ) also follows roughly a power law with a different exponent than in regime (I). We find for T$_{i}$ = 5000 K, T$_{f}$ = 2500 K, 2750 K and q = 1 . 7 ˚ A − $^{1}$, 2 . 7 ˚ A − 1 µ ≈ 0 . 35 with variations of the order of 0 . 08 depending on T$_{f}$ , particle type, and q . Best power law fits are for T$_{i}$ = 3760 K, T$_{f}$ = 2500K with µ ranging from µ = 0 . 55/0 . 57 for q = 1 . 7 ˚ A − 1 to µ = 0 . 69/0 . 63 for q = 6 . 6 ˚ A − 1 and for Si/O atoms. Kob and Barrat find for the binary Lennard-Jones system also a power law for t Cq r ( t$_{w}$ ), however, with µ = 0 . 882 [16]. Similar to Grigera et al. [47] we find that the transition from small 

