A schematic representation
of the IPAP-FESTA
pulse sequence is shown in
Figure 1. It can be described as a doubly selective modulated
echo followed by a TOCSY transfer, similar to MODO-FESTA.
35 (link) The resulting spectrum shows only
1H signals that are in the same spin system as that of a specific
19F site. IPAP-FESTA contains four variations of the modulated
echo, resulting in the acquisition of two complementary sets of interleaved
IP and AP data. Within each data set, modulated and unmodulated data
are acquired by changing the phase of the excitation 90°
1H pulse (ϕ
1 =
x on odd-numbered
scans, ϕ
1= −
x on even-numbered
scans) and using different arrangements of
19F selective
iBURP pulses and delays in odd- and even-numbered scans. The delay
Δ is set to 1/2
JHF for A
nX and A
nX
3 spin systems and 1/4
JHF for A
nX
2 spin systems, where
n is the number of equivalent protons and
JHF is the heteronuclear coupling constant between the selected fluorine
and proton(s). Note that the second iBURP
19F pulse is
time-reversed with respect to the first, to refocus any
JHF evolution that occurs during the first pulse.
33 (link),39 (link) In each data set, identical signals are obtained in odd- and even-numbered
scans for the selected protons, while all other protons yield equal
but opposite phases and, therefore, are suppressed by summing the
two scans. Field gradient pulses flank the selective
1H
shaped pulse for coherence transfer pathway selection. A hard 90°
1H pulse is applied after the modulated echo, with the phase
ϕ
2 of the pulse depending on whether IP (ϕ
2 =
x) or AP (ϕ
2 = −
x) data are being acquired. For the TOCSY transfer, DIPSI-2
is used as the isotropic mixing element,
40 (link) transferring the IP or AP magnetization from the selected
1H signal to all other spins within the same spin system. Zero-quantum
suppression elements are applied on either side of the DIPSI-2 element,
together with a purge gradient pulse, to suppress the effects of zero-quantum
coherences and of unwanted transverse magnetization.
41 (link) A final 90°
x1H pulse transfers all desired magnetization to the transverse plane
for observation. An additional phase-cycled 90°
19F pulse is applied simultaneously to the 90°
1H pulse
in IP-MODO-FESTA, to ensure that any remaining AP contributions are
suppressed before data acquisition and to give pure IP signals. The
result is that only proton signals from the selected
1H–
19F spin system, IP or AP with respect to the
JHF coupling to the specified
19F survive with
any other signals being suppressed. SRI-FESTA
34 (link) could potentially be used instead of MODO-FESTA; however the higher
sensitivity of the latter is advantageous when analyzing dilute mixtures
such as the fluticasone propionate mixture described here. Further
details are provided in the
SI.
Mycroft C., Dal Poggetto G., Barbosa T.M., Tormena C.F., Nilsson M., Morris G.A, & Castañar L. (2023). Rapid Measurement of Heteronuclear Coupling Constants in Complex NMR Spectra. Journal of the American Chemical Society, 145(36), 19824-19831.