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TROSY-HNCO

Fig. 4. The HNCO-TROSY experiment for recording solely interresidual 1HN, 15N, 13C correlations in 13C/15N/2H labelled proteins. All 90° (180°) pulses for the 13C and 13C spins are applied with a strength of 2/ /l5 (p/ /3), where 2 is the frequency difference between the centres of the 13C and 13Ca regions. All 13Ca pulses are applied off-resonance with phase modulation by Q. A = 1/(4/hn) Tn = l/(4/NC ) S = gradient + field recovery delay 0 < k < TN/z2,max- Phase cycling i = y 4>2 = x, — x + States-TPPI 03 = x 0rec = x, — x. Fig. 4. The HNCO-TROSY experiment for recording solely interresidual 1HN, 15N, 13C correlations in 13C/15N/2H labelled proteins. All 90° (180°) pulses for the 13C and 13C spins are applied with a strength of 2/ /l5 (p/ /3), where 2 is the frequency difference between the centres of the 13C and 13Ca regions. All 13Ca pulses are applied off-resonance with phase modulation by Q. A = 1/(4/hn) Tn = l/(4/NC ) S = gradient + field recovery delay 0 < k < TN/z2,max- Phase cycling </>i = y 4>2 = x, — x + States-TPPI 03 = x 0rec = x, — x.
The magnetization has now been successfully transferred from the HN spin to the intraresidual and sequential 13C spins or alternatively to the interresidue 13C spin either using HNCA-TROSY or HNCO-TROSY schemes, respectively. It is inevitable that the HNCO-TROSY spectrum cannot be used for the sequential assignment alone because it does not bridge two sequential N shifts through common carbonyl carbon frequency. The... [Pg.256]

In the alternative approach, the HN(i), 15N( j, 13C (i/i— 1) correlations in the HNCA-TROSY spectrum can be supplemented with the data from the HN(CO)CA-TROSY experiment72 73 yielding solely 11 IN(/), 15N( ), 13C (i- 1) correlations. To this end, the HNCO-TROSY experiment is extended with the 13C —> 13C INEPT step, which utilizes rather large (ca. 51-55 Hz) one-bond scalar coupling between the 13C and 13C spins in order to transfer magnetization from the 13C (< — 1) nucleus further to the 13C ( — 1) spin. [Pg.259]

Fig. 23. Coherence transfer efficiency as a function of delay 2Tn f°r the HNCO-TROSY scheme. Following parameters were used [Eq. (12)] T 2,i5n = 50 ms, VNc = 15 Hz. Fig. 23. Coherence transfer efficiency as a function of delay 2Tn f°r the HNCO-TROSY scheme. Following parameters were used [Eq. (12)] T 2,i5n = 50 ms, VNc = 15 Hz.
HNfz) connectivities with good sensitivity, excluding serines, threonines, leucines, and glycines (and probably valines and prolines). Thus, the use of HNCO-TROSY/HN(CA)CO-TROSY experiment pair can be very useful in assigning high molecular weight proteins. [Pg.292]

D HCN-based 2D HNCO-TROSY-based 2D HN(CO)CA-TROSY-based 2D HNCA-TROSY-based 2D HNCO-based... [Pg.351]

The HNCA-TROSY experiment can be readily extended to correlate the 13C spin of the preceding residue with intraresidual 11 IN(/), 15N(i), and 13C° (/ ) frequencies. This kind of four-dimensional HNCO CA-TROSY experiment (Fig. 7) was recently introduced by Konrat et al.79 The coherence flows through the following pathway... [Pg.264]

The set of four-dimensional (HNCO, iCA, HNCOCA and HNCACO) TROSY experiments has been successfully applied in the assignment of several large proteins.12,25,26 These three experiments are able to resolve... [Pg.292]

Residual dipolar couplings 3D TROSY-HNCO-based... [Pg.307]


See other pages where TROSY-HNCO is mentioned: [Pg.256]    [Pg.258]    [Pg.287]    [Pg.288]    [Pg.290]    [Pg.293]    [Pg.215]    [Pg.216]    [Pg.217]    [Pg.107]    [Pg.340]    [Pg.589]    [Pg.256]    [Pg.258]    [Pg.287]    [Pg.288]    [Pg.290]    [Pg.293]    [Pg.215]    [Pg.216]    [Pg.217]    [Pg.107]    [Pg.340]    [Pg.589]    [Pg.26]    [Pg.257]    [Pg.264]    [Pg.266]    [Pg.269]    [Pg.287]    [Pg.293]    [Pg.89]    [Pg.187]    [Pg.234]    [Pg.45]    [Pg.53]    [Pg.313]    [Pg.297]    [Pg.314]    [Pg.1367]    [Pg.861]    [Pg.884]    [Pg.114]    [Pg.114]    [Pg.347]    [Pg.365]   
See also in sourсe #XX -- [ Pg.288 ]




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