Pulse sequences for 3D SOFAST HMQC-NOESY-HMQC with the following frequency labeling combinations: a) N(F1)-N(F2)HN(F3), b) CM(F1)-N(F2)HN(F3), c) CM(F1)-CM(F2)HM(F3), and d) N(F1)-CM(F2)HM(F3). The smaller and larger 1H shaped pulses are 1.69 ms long 90° PC9_4_90 (Smith 2001) and 1.15 ms long 180° REBURP (Geen and Freeman 1991), respectively. The flip angle α (110° to 90°, depending on the value of d1 and the experiment type) of the shaped pulse after τmix should be optimized (see text). Depending on the sequence, the offsets of the 1H shaped pulses are −3,230 Hz (at 0.9 ppm) for methyl type pulses and 3,230 Hz (at 8.5 ppm) for amides. The narrow bars represent 90° hard pulses. The shaped pulse on 13C channel represents a 500 µs long 180° smoothed CHIRP. (Hwang et al. 1997) The spectral centers of 15N, 13C, and 1H dimensions are at 118.0, 16.5, and 4.7 ppm, respectively. The delays are: d1 = 0.2 sec, Δ1 = 1/(2×1JCH3) = 4.0 ms, Δ2 = 1/(2×1JNH) = 5.2 ms τmix = 0.3 sec. The phase cycling for X-XH-type are φ1 = (x, −x), φ2 = (x, −x, −x, x), φrec = (x, −x, −x, x) and for X-YH-type are φ1 = (x, −x), φ2 = (x, −x, −x, x), φ3 = 4(x), 4(−x), φrec = (x, −x, −x, x, −x, x, x, −x). Bruker decoupling scheme bi_garp_2pl is used. The quadrature detections in t1 and t2 dimensions are acquired via States-TPPI of φ1 and φ2, respectively. The durations and strengths of the gradients are G1 = (1 ms, 15 G/cm), G2 = (1 ms, 5 G/cm).