Coupling constants can provide useful supplementary information in the structural analysis of nucleic acids and proteins. It is often difficult, however, to determine their values as the large linewidths tend to obscure the multiplet patterns. For this reason it is desirable to interpret reduced rather than full multiplet effects in COSY spectra (I, 2). To this end several alternative methods have been developed. These include /3COSY (2), bilinear COSY (3), E.COSY (4), and z-COSY (5). The z-COSY and E.COSY techniques both yield spectra with reduced multiplet patterns and pure absorption lineshapes for all peaks in the spectrum. While full suppression of the undesired multiplet components can be achieved with E.COSY, the extent of suppression in z-COSY depends on the choice of flip angle for the two mixing pulses. The effects of strong coupling, however, are not as severe for z-COSY as it uses only small pulses (6). In this paper we demonstrate the application of z-COSY to macromolecules using the DNA hexamer 5’d(GCATGC)2 as an example and discuss the effects resulting from incomplete suppression of the undesired multiplet components of the cross peaks. Further, we show that in order to obtain a spectrum of sufficient quality for the measurement of coupling constant, the z-COSY technique should be applied in a modified manner with respect to the suppression of zero-quantum coherences. The basic pulse sequence for z-COSY is 90”-t,+?-7,-&t,. The phase cycling must be designed in such a manner that coherences of the order p = t1 are retained during t, and only populations and zero-quantum coherences are selected during the delay 7,. In the case of macromolecules, the application of the normal NOESY phase-cycle selecting coherences of the order p = 0 f 4n (n = integer) during the delay T, is sufficient. To obtain a z-COSY spectrum with pure absorption lineshapes it is necessary to suppress the zero-quantum transitions (ZQT) appropriately. Because of the intrinsic similarity of the pulse sequences, the methods used for NOESY experiment (7-9) can also be applied to z-COSY. In the original description of the z-COSY experiment (5), zero-quantum suppression was achieved by a random variation of the delay between the two mixing pulses. Unfortunately, this introduces noise into the spectrum due to the effective smearing of the zero-quantum peaks along the w1 axis and the generation oft, noise arising from the random variation in the relaxation of the diagonal peaks
Read full abstract