2010
DOI: 10.1016/j.cplett.2010.07.037
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Indirect high-resolution detection for quadrupolar spin-3/2 nuclei in dipolar HMQC solid-state NMR experiments

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Cited by 33 publications
(15 citation statements)
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“…40,[55][56][57] More recently, its broadbandedness has also been exploited for the detection of correlations to ultra-wideline and isotropic spectra of heavy spin-1/2 nuclei 58,59 as well as satellite transitions of quadrupolar nuclei. 60,61 Despite the abovementioned advantages, the D-RINEPT and D-HMQC techniques are limited by the lack of radiofrequency (RF) power flexibility of non-γ-encoded heteronuclear dipolar recoupling sequences. While a near continuum of γ-encoded heteronuclear recoupling sequences (that also decouple homonuclear dipolar interactions) exists with both high-and lowradiofrequency (RF) requirements, non-γ-encoded heteronuclear dipolar recoupling sequences are limited to low RF power (νRF = 2νR or 4/3νR, where νR denotes the MAS spinning frequency).…”
Section: Introductionmentioning
confidence: 99%
“…40,[55][56][57] More recently, its broadbandedness has also been exploited for the detection of correlations to ultra-wideline and isotropic spectra of heavy spin-1/2 nuclei 58,59 as well as satellite transitions of quadrupolar nuclei. 60,61 Despite the abovementioned advantages, the D-RINEPT and D-HMQC techniques are limited by the lack of radiofrequency (RF) power flexibility of non-γ-encoded heteronuclear dipolar recoupling sequences. While a near continuum of γ-encoded heteronuclear recoupling sequences (that also decouple homonuclear dipolar interactions) exists with both high-and lowradiofrequency (RF) requirements, non-γ-encoded heteronuclear dipolar recoupling sequences are limited to low RF power (νRF = 2νR or 4/3νR, where νR denotes the MAS spinning frequency).…”
Section: Introductionmentioning
confidence: 99%
“…Therefore, the quest for increased resolution in the quadrupolar dimension of 2D correlation spectra under MAS has led over the past years to the development of several sequences, which all derive from the alliance of a multiple-quantum (MQ) 11 or satellite transition (ST) 12 MAS quadrupolar filter with one of the above-mentioned HETCOR schemes. These filters were first combined with HETCOR experiments relying either on single coherence transfers, such as classical CP (MQ-CP-HETCOR, [13][14][15] and ST-CP-HETCOR) 16 or J-R-INEPT (MQ-J-R-INEPT), 4,15,17 or on two consecutive coherence transfers, such as the MQ-J-HMQC 18 and HMQC-ST 19 experiments. However, (i) CP transfers involving quadrupolar nuclei suffer from lack of robustness, as mentioned above, 6 (ii) the MQ-J-HMQC experiment requires a prohibitively long 3D acquisition and (iii) HMQC-ST is only applicable to spin-3/2 nuclei (for other spin values, the phase cycling can't separate the interactions).…”
Section: Introductionmentioning
confidence: 99%
“…However, (i) CP transfers involving quadrupolar nuclei suffer from lack of robustness, as mentioned above, 6 (ii) the MQ-J-HMQC experiment requires a prohibitively long 3D acquisition and (iii) HMQC-ST is only applicable to spin-3/2 nuclei (for other spin values, the phase cycling can't separate the interactions). 19 Presently, the most robust high-resolution experiment adapted to quadrupolar nuclei with any halfinteger spin value is thus the MQ-J-R-INEPT sequence. 4,15,17 However, depending on the sample, this J-mediated experiment may present a low signal to noise (S/N) ratio when the signal decay resulting from coherent and incoherent processes is faster than the dephasing under the J coupling.…”
Section: Introductionmentioning
confidence: 99%
“…The t 1 -noise hampers the observation of 2D D-HMQC and D-HMQC filtered 1D 1 H NMR at 80 kHz. Active synchronization of excitation and reconversion sequence to sample spinning should reduce the t 1 -noise [13,26]. Alternatively, this problem could be solved by continuously notifying the instantaneous spinning frequency and updating the pulse sequence timing.…”
Section: Resultsmentioning
confidence: 98%