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21-24 for which partial alignment could be retained even after long delay time. However, the temporal profile shown in Figure 4 refers to the reaction products and thus is the result of a cumulative depolarization effect (i.e., not the instantaneous time-dependent alignment of the reactants; see eqs 4 and 5) over the delay time of two lasers. In addition, possible collision-induced depolarization eff ects that tend to damp the oscillatory behaviors cannot be completely ruled out at longer delay time even under the crossed-beam conditions. In conjunction with the fact the observed temporal profiles do not show any oscillation (Figure 4), we surmise that using a more complicated, oscillatory decay form will not significantly affect the estimate made in this work.
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