The J′ dependencies of energy and line width of the 23 Na 39 K B 1 Π(V′ ) 30-43, J′) r X 1 Σ + (V′′ ) 2, J′′) transitions are measured up to the breaking-off points, where NaK dissociates to the Na(3s 2 S 1/2 ) + K(4p 2 P 3/2 ) atoms. Line broadenings are observed for transitions to the B 1 Π(V′ ) 30, J′ g 42), (V′ ) 31, J′ g 35), (V′ ) 32, J′ g 27), (V′ ) 33, J′ g 14), and (V′ g 34, all J′) levels, and are attributed to the predissociation via the c 3 Σ + state to the Na(3s 2 S 1/2 ) + K(4p 2 P 1/2 ) atoms. The (V′, J′) dependence of the predissociation threshold is attributed to the potential barrier due to rotation. Below and near the threshold, a series of the perturbation centers which converge to the predissociation threshold is observed for each V′, and the perturbing state is identified as the c 3 Σ + state. Rotational perturbations are observed also above the predissociation threshold, and the perturbing state is identified as the b 3 Π 1 state. The line widths are observed to change drastically around the maximum perturbation, and this is identified as originating from the interference effect which arises because both the B 1 Π and b 3 Π 1 states interact with the dissociative continuum of the c 3 Σ + state. In the transitions to levels near the breaking-off points of the B 1 Π(V′ g 37), the line splittings into two lines are observed for each J′. This splitting is identified as originating from the S-uncoupling interaction between the B 1 Π and b 3 Π states at a long internuclear distance. Similar line splittings are observed for the B 1 Π(V′ ) 30, all J′) levels, but are not observed for V′ ) 31-36. An accidental coincidence of the level energies of the B 1 Π(V′ ) 30) and b 3 Π(V) levels is presumed, and the origin of the line splitting is identified as the S-uncoupling interaction. This is confirmed by the analysis of the hyperfine structures observed for the split lines.