Figure 3
Decomposed PNS kick velocities for models L2.25 (top panel), L2.3 (middle panel) and L2.4 (bottom panel), obtained by integrating equation (4) from bounce. We have inverted the velocities for the L2.3 run. The dot–dashed black curve depicts the PNS velocity computed using the centroid of the density, while the solid red curve shows the contributions to the kick from momentum flux (long-dashed blue curve), gravity (dashed green curve) and pressure (dot–dashed pink curve). In each run, the PNS is still accelerating at more than 500 km s−2 at the end of the calculation, and this acceleration is dominated by the gravitational term.

Decomposed PNS kick velocities for models L2.25 (top panel), L2.3 (middle panel) and L2.4 (bottom panel), obtained by integrating equation (4) from bounce. We have inverted the velocities for the L2.3 run. The dot–dashed black curve depicts the PNS velocity computed using the centroid of the density, while the solid red curve shows the contributions to the kick from momentum flux (long-dashed blue curve), gravity (dashed green curve) and pressure (dot–dashed pink curve). In each run, the PNS is still accelerating at more than 500 km s−2 at the end of the calculation, and this acceleration is dominated by the gravitational term.

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