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Table 2

Simulation results presented according to the four-population classification.

φσ v0 Etot m1 E1 m2 E2 mpw Epw Npw msr Esr Nsr
[m   s-1] [J] [kg] [J] [kg] [J] [kg] [J] [kg] [J]
0.00 10.0 5.81 3.56 5.64 5 × 10-5 1 × 10-4 5 × 10-3 3 × 10-3 17 2 × 10-3 0.17 158
0.01 10.0 5.99 3.55 5.61 3 × 10-4 7 × 10-4 3 × 10-3 0.01 36 0.01 0.36 610
0.02 10.0 6.72 1.62 2.75 0.52 0.82 1.39 2.30 290 0.04 0.84 2854
0.03 10.0 7.35 1.25 2.28 0.49 0.80 1.75 3.03 588 0.07 1.24 6043
0.04 10.0 7.80 0.55 0.91 0.35 0.75 2.55 4.64 1057 0.11 1.50 9292
0.05 10.0 9.09 0.43 0.71 0.32 0.54 2.56 5.54 3056 0.25 2.30 20657
0.00 12.5 9.78 1.92 4.47 0.31 0.78 1.33 4.14 123 0.01 0.39 861
0.01 12.5 10.12 1.74 4.42 0.67 1.83 1.13 2.87 157 0.02 1.00 1650
0.02 12.5 11.93 1.17 3.73 0.23 0.52 2.07 5.45 984 0.08 2.23 6882
0.03 12.5 13.24 0.72 2.40 0.21 0.74 2.47 6.91 1865 0.16 3.19 13285
0.04 12.5 14.29 0.59 2.03 0.18 0.40 2.54 7.90 3180 0.25 3.96 20402
0.05 12.5 19.20 0.15 0.38 0.09 0.27 2.68 11.13 10578 0.65 7.42 52478

Notes. The subscripts “1”, “2”, “pw”, “sr”, and “tot” denote the largest and second largest fragment, the power-law, sub-resolution, and total fragment population, respectively. The quantities E, m, and N are the total energy, the mass, and the number of fragments, respectively. The standard deviation for the inhomogeneity Gaussian distribution is given by φσ and the impact velocity by v0.

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