Experimental scheme for the 2D
hJNN-correlation-[15N,1H]-TROSY
experiment used to correlate the chemical shifts of pairs of hydrogen
bond-related 15N spins and to measure
hJHN. On the lines marked
1H, 15N, and 13C, narrow and wide
bars stand for nonselective 90° and 180° radio frequency pulses,
respectively, with the carrier frequencies at 12, 190, and 145 ppm,
respectively. The delays are τ1 = 2.7 ms,
τ2 = 18 ms, and τ3 = τ2 −
τ1. The line marked PFG indicates the pulsed magnetic
field gradients applied along the z axis:
G1, amplitude 30 G/cm, duration 1 ms; G2, 42
G/cm, 1 ms; G3, 45 G/cm, 1 ms; G4, 40
G/cm, 1 ms; and G5, 48 G/cm, 1 ms. Two data sets, I and
II, are measured in the interleaved manner with the following phase
cycling schemes: (I), φ1 = {−x, x}; φ2
= {2(−x),2x}; ψ1 = {4y,4(−y)};
ψ2(receiver) = {y,−y,−y, y,−y, y,y,−y}; (II),
φ1 = {−y, y}; φ2 = {2(−y),2y};
ψ1 = {4(−x),4x}; ψ2(receiver) =
{−x, x,x,−x, x,−x,−x, x}; x on all other pulses. For both data
sets, quadrature detection in the t1
dimension is obtained by using States-TPPI (38) by simultaneously
incrementing each of the phases φ2 and ψ2
by 90°. The transfer of 15N magnetization to
1H for detection of single transition-to-single transition
polarization transfer (5) was used. Fourier transformation of the sum
and difference of the two data sets results in two 2D
hJNN-
correlation-[15N,1H]-TROSY spectra in which
the relative cross-peak positions are determined in E.COSY manner by
the chemical shifts and the scalar-coupling constants (27–30). For
example, both the direct and the relayed correlation cross-peaks that
appear in the two spectra are shifted by
1JHN along
ω2(1H). Along
ω1(15N), the direct peaks also are shifted by
1JHN, but the separation
of the relayed cross-peaks is determined exclusively by
hJHN. To enhance the signals of
rapidly exchanging imino protons, water saturation is minimized by
keeping the water magnetization along +z during the entire experiment,
using the water-selective 90° pulses indicated by curved shapes on
the line 1H.