The effect on the annihilation location for (a) three postulated initial energy distributions. As the trap depth is about 540 mK, most, but not all, of the anti-atoms beyond 540 mK will be untrapped31,38. (b) The F=1 time-reversed CDF of the simulated annihilations during the magnet shutdown for the three distributions, following the labelling in (a). The black points plot the time-reversed CDF of the experimental events (which mainly appear as a band behind the red Maxwellian line.) The event data agrees well with the Maxwellian distribution. (c) A typical distribution in y of late annihilations (those occurring between 20 and 22 ms). (d) The reverse cumulative average, 〈y|t〉, for the three distributions, as defined in the text. For (c) and (d), F=80; as expected, the plotted lines in these last two graphs show little dependence on the postulated energy distribution.