Data for Fig. 7 of J. Phys. A 51 (2018) 495002

Same as Figure 4 but for fields along the line $\log(Z_2H_2/M_0)\equiv 0.4\log(Z_1H_1/M_0)-2.58$. Transitions are observed at fields where the quarks and antiquarks condense, i.e.\ from the low density phase of non-interacting anyons into the collective state described by the $SU(3){N_f=2}/SU(2){N_f=2}$ coset CFT at and later into a phase whose low energy description is in terms of the $SU(3)_{N_f=2}$ WZNW model. The dashed-dotted lines indicate the corresponding central charges.