BR PT TY LAB PAR(1) L2-NORM MAX U(1) ... 1 15 UZ 2 1.700000E+00 3.836401E-01 4.890015E-01 1 16 LP 3 1.711574E+00 3.922135E-01 5.442385E-01 1 19 UZ 4 1.600000E+00 4.329404E-01 7.769491E-01 1 31 UZ 5 1.000000E+00 4.808488E-01 1.083298E+00 1 86 UZ 6 -9.664802E-10 5.158463E-01 1.258650E+00contains the label of a limit point (ILP was set to 1 in c.rev.3, which corresponds to a ``coalescence'' of two reversible homoclinic orbits. The two solutions on either side of this limit point are displayed in Figure 26.3. The computation ends in a no-convergence point. The solution here is depicted in Figure 26.4. The lack of convergence is due to the large peak and trough of the solution rapidly moving to the left as (cf. ChSp:93).
Continuing from the initial solution in the other parameter direction
BR PT TY LAB PAR(1) L2-NORM MAX U(1) ... 1 7 UZ 8 1.600000E+00 3.701709E-01 3.836833E-01 1 33 UZ 9 9.999980E-01 3.614405E-01 1.775035E-01 1 93 UZ 10 -7.819855E-06 3.713007E-01 4.698309E-02which again ends at a no convergence error for similar reasons.