Fig. 14
τ(3889) for the two main kinematic components presented in Fig. 19 of Paper I derived from the fits to relations presented by Robbins (1968) for Te = 10 000 K. Left: narrow kinematic component and ω = 0. Right: broad kinematic component and ω = 3. The τ(3889) map for this component using the relation for ω = 0 (not shown) displays the same structure but with values ~4–6 times lower.
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