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. 2010 May 13;368(1918):2221–2236. doi: 10.1098/rsta.2010.0038

Figure 9.

Figure 9.

Temporary wave detachment (a=0.8 and b=0.06). According to figure 5 (with R=3 and E=7), there is (to accuracy ±T/96) no unpinning window for these parameters. But there are pulse times for which one end of the FFP wave temporarily detaches from the obstacle. One of these cases is shown here. Its timing is indicated by a circle in figure 6. The time evolution looks similar to figure 8a,c. Apparently, these cases have converged and eliminated the unpinning window in between.