Figure 1
Light curves without self-absorption and electron cooling, leaving only critical frequency νm. The light curves are calculated at observer frequencies 1.4 × 109 Hz (upper light curves) and 5 × 1017 Hz (lower light curves), to ensure they are on different sides of νm. Results for 5 × 1017 Hz have been multiplied by a scaling factor of 100. Aside from results from spherical flow, results from hard-edged jets with half-opening angles of 10°, 15° and 20° are plotted. The new predicted jet break times (equation 7 in the text) are indicated by dots connected to the lower edge of the plot, old predictions (equation 4 in the text) connect to the upper edge of the plot.

Light curves without self-absorption and electron cooling, leaving only critical frequency νm. The light curves are calculated at observer frequencies 1.4 × 109 Hz (upper light curves) and 5 × 1017 Hz (lower light curves), to ensure they are on different sides of νm. Results for 5 × 1017 Hz have been multiplied by a scaling factor of 100. Aside from results from spherical flow, results from hard-edged jets with half-opening angles of 10°, 15° and 20° are plotted. The new predicted jet break times (equation 7 in the text) are indicated by dots connected to the lower edge of the plot, old predictions (equation 4 in the text) connect to the upper edge of the plot.

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