Abstract

Half-integer spin quadrupolar nuclei are the only magnetic isotopes for the majority of the chemical elements. Therefore, the transfer of polarization from protons to these isotopes under magic-angle spinning (MAS) can provide precious insights into the interatomic proximities in hydrogen-containing solids, including organic, hybrid, nanostructured and biological solids. This transfer has recently been combined with dynamic nuclear polarization (DNP) in order to enhance the NMR signal of half-integer quadrupolar isotopes. However, the cross-polarization transfer lacks robustness in the case of quadrupolar nuclei, and we have recently introduced as an alternative technique a -RINEPT (through-space refocused insensitive nuclei enhancement by polarization transfer) scheme combining a heteronuclear dipolar recoupling built from adiabatic pulses and a continuous-wave decoupling. This technique has been demonstrated at 9.4 T with moderate MAS frequencies, -15 kHz, in order to transfer the DNP-enhanced H polarization to quadrupolar nuclei. Nevertheless, polarization transfers from protons to quadrupolar nuclei are also required at higher MAS frequencies in order to improve the H resolution. We investigate here how this transfer can be achieved at and 60 kHz. We demonstrate that the -RINEPT sequence using adiabatic pulses still produces efficient and robust transfers but requires large radio-frequency (rf) fields, which may not be compatible with the specifications of most MAS probes. As an alternative, we introduce robust and efficient variants of the -RINEPT and PRESTO (phase-shifted recoupling effects a smooth transfer of order) sequences using symmetry-based recoupling schemes built from single and composite pulses. Their performances are compared using the average Hamiltonian theory and experiments at T on -alumina and isopropylamine-templated microporous aluminophosphate (AlPO-14), featuring low and significant H-H dipolar interactions, respectively. These experiments demonstrate that the H magnetization can be efficiently transferred to Al nuclei using -RINEPT with (27090) recoupling and using PRESTO with (180) or (27090) schemes at or 62.5 kHz, respectively. The -RINEPT and PRESTO recoupling schemes complement each other since the latter is affected by dipolar truncation, whereas the former is not. We also analyze the losses during these recoupling schemes, and we show how these magnetization transfers can be used at kHz to acquire in 72 min 2D HETCOR (heteronuclear correlation) spectra between H and quadrupolar nuclei, with a non-uniform sampling (NUS).

Highlights

  • Quadrupolar nuclei with a nuclear spin quantum number S = 3/2, 5/2, 7/2 or 9/2 are the only NMR-active isotopes for over 60 % of the chemical elements of the first six periods of the periodic table, including six of the eight most abundant elements by mass in the Earth’s crust: O, Al, Ca, Na, Mg and K (Ashbrook and Sneddon, 2014)

  • We analyze the losses during these recoupling schemes, and we show how these magnetization transfers can be used at νR = 62.5 kHz to acquire in 72 min 2D HETCOR spectra between 1H and quadrupolar nuclei, with a non-uniform sampling (NUS)

  • crosspolarization under MAS (CPMAS) experiments require a careful adjustment of the rf field applied to the quadrupolar isotope in order to fulfill the Hartmann–Hahn conditions, (S+1/2)ν1S+εν1H = nνR, where ν1S and ν1H denote the amplitudes of the rf fields applied to the S quadrupolar isotope and to the protons, respectively; ε = ±1, n = ±1, or ±2; and νR denotes the magic-angle spinning (MAS) frequency, while avoiding the rotary resonance recoupling (R3) ν1S = pνR/(S + 1/2) with p = 0, 1, 2 and 3 (Amoureux and Pruski, 2002; Ashbrook and Wimperis, 2009)

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Summary

Introduction

More recently, the through-space refocused INEPT (denoted RINEPT hereafter) (Nagashima et al, 2020; Giovine et al, 2019) These schemes benefit from higher robustness than CPMAS since they do not employ a spin-lock on the quadrupolar channel but instead a limited number (two or three) of CT selective pulses. (ii) continuous-wave (CW) irradiations during the windows, and (iii) composite π/2 and π pulses on the 1H channel, in order to limit the losses due to 1H–1H interactions and improve the transfer efficiency at moderate MAS frequencies (Nagashima et al, 2020, 2021) This novel RINEPT variant, denoted RINEPT-CWc-SR421(tt), is more efficient than PRESTO and CPMAS at νR ≈ 12.5 kHz, and it has been combined with DNP to detect the NMR signals of quadrupolar nuclei with small dipolar coupling with protons, including the low-γ isotopes, such as 47,49Ti, 67Zn or 95Mo, and unprotonated 17O nuclei.

Single-quantum heteronuclear dipolar recoupling
Selection of the recoupling sequence
Zero-quantum heteronuclear dipolar recoupling
D-RINEPT-CWc sequence
Simulation parameters
Optimal adiabatic recoupling
Samples and experimental conditions
AlPO4-14
Decay of transverse 1H magnetization during recoupling
Findings
Conclusions
Full Text
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