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. Author manuscript; available in PMC: 2017 Dec 1.
Published in final edited form as: J Biomol NMR. 2016 Nov 23;66(4):259–271. doi: 10.1007/s10858-016-0074-5

Fig. 3.

Fig. 3

Pulse sequences in top panels are for diagonal-free Aro-Methyl 3D SOFAST HMQC-NOESY-HMQC (a) and reference 3D HSQC-NOESY-HMQC sequence (b). Frequency labeling is CAro(F1)-CM(F2)HM(F3). Top a): the smaller and larger 1H shaped pulses are 1.69 ms long 90° PC9_4_90 and 1.15 ms long 180° REBURP, respectively. The first and second vertical arrows on 1H and 13C channels indicate the 1H(13C) carrier frequency setting to 8.5 ppm (122 ppm) and 4.7 ppm (17.5 ppm), respectively. The offsets of 1H shaped pulses before and after τmix are 0 (at 4.7 ppm) and −3,230 Hz (at 0.9 ppm), respectively. The narrow bars represent 90° hard pulses. The spectral centers of 13C(F1), 13C(F2), 1H(F3) dimensions are at 122.0, 16.5, and 4.7 ppm, respectively. The delays are: d1 = 200 ms, Δ1 = 3.1 ms, Δ2 = 4.0 ms, τmix = 300 ms. The phase cycling are: φ1 = (x, −x), φ2 = (x, −x, −x, x), φ3 = 4(x), 4(y), φ4 = 8(x), 8(−x), φrec = (x, −x, −x, x, −x, x, x, −x, −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). Top (b): reference WATERGATE (W5’) 3D HSQC-NOESY-HMQC pulse sequence used for the S/N comparison. The filled narrow and wide bars represent 90° and 180° hard pulses, respectively. The open narrow (41.6 µs) and wide (37.2 µs) bars on 13C channel represent 90° and 180° soft pulses, respectively, that have null excitation at an offset of 109 ppm. 13C shaped pulses are 423 µs IBURP2.1000 180° pulses (Geen and Freeman 1991). The first and second vertical arrows indicate the 13C carrier frequency setting to 122.0 ppm and 17.5 ppm (centers of aromatic and methyl 13C chemical shifts), respectively. The distances between 3-9-19 W5’ pulses are 148 µs. The delays are: d1=1.0 sec, Δ1 = 3.1 ms, Δ2 = 4.0 ms, δ = t1(0) + 2*pw (initial t1 value and 1H 180° pulse width), τmix = 0.3 sec. The phase cycling is: φ1 = (x, −x, −x, x), φ2 = (x, −x), φ3 = 4(x), 4(y), 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, 10 G/cm), G2 = (1 ms, 5 G/cm), G3 = (2 ms, 10 G/cm). Bottom panels show comparison of pure NOE F2(CM)-F3(HM) planes run using the FliT-FliJ complex sample (see main text Materials and Methods) that contained both 1H-13C methyl and aromatic labels. Mixing time was 0.3 s, d1 = 0.2 s, and 90 degrees variable angle pulse (α) for SOFAST version.