<strong class="journal-contentHeaderColor">Abstract.</strong> <span id="page448"/>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 <span class="inline-formula"><i>D</i></span>-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 9.4âT with moderate MAS frequencies, <span class="inline-formula"><i>ν</i><sub>R</sub>â10</span>â15âkHz, in order to transfer the DNP-enhanced <span class="inline-formula"><sup>1</sup></span>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 <span class="inline-formula"><sup>1</sup></span>H resolution. We investigate here how this transfer can be achieved at <span class="inline-formula"><i>ν</i><sub>R</sub>â20</span> and 60âkHz. We demonstrate that the <span class="inline-formula"><i>D</i></span>-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 <span class="inline-formula"><i>D</i></span>-RINEPT and PRESTO (phase-shifted recoupling effects a smooth transfer of order) sequences using symmetry-based recoupling schemes built from single and composite <span class="inline-formula"><i>Ï</i></span> pulses. Their performances are compared using the average Hamiltonian theory and experiments at <span class="inline-formula"><i>B</i><sub>0</sub>=18.8</span>âT on <span class="inline-formula"><i>γ</i></span>-alumina and isopropylamine-templated microporous aluminophosphate (AlPO<span class="inline-formula"><sub>4</sub></span>-14), featuring low and significant <span class="inline-formula"><sup>1</sup></span>Hâ<span class="inline-formula"><sup>1</sup></span>H dipolar interactions, respectively. These experiments demonstrate that the <span class="inline-formula"><sup>1</sup></span>H magnetization can be efficiently transferred to <span class="inline-formula"><sup>27</sup></span>Al nuclei using <span class="inline-formula"><i>D</i></span>-RINEPT with <span class="inline-formula"><math xmlns="http://www.w3.org/1998/Math/MathML" id="M17" display="inline" overflow="scroll" dspmath="mathml"><mrow><mi mathvariant="normal">SR</mi><msubsup><mn mathvariant="normal">4</mn><mn mathvariant="normal">1</mn><mn mathvariant="normal">2</mn></msubsup></mrow></math><span><svg:svg xmlns:svg="http://www.w3.org/2000/svg" width="28pt" height="16pt" class="svg-formula" dspmath="mathimg" md5hash="bfb1b3a831bd4cb203459286d6469a1c"><svg:image xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="mr-2-447-2021-ie00001.svg" width="28pt" height="16pt" src="mr-2-447-2021-ie00001.png"/></svg:svg></span></span>(270<span class="inline-formula"><sub>0</sub></span>90<span class="inline-formula"><sub>180</sub></span>) recoupling and using PRESTO with <span class="inline-formula"><math xmlns="http://www.w3.org/1998/Math/MathML" id="M20" display="inline" overflow="scroll" dspmath="mathml"><mrow><mi mathvariant="normal">R</mi><msubsup><mn mathvariant="normal">22</mn><mn mathvariant="normal">2</mn><mn mathvariant="normal">7</mn></msubsup></mrow></math><span><svg:svg xmlns:svg="http://www.w3.org/2000/svg" width="27pt" height="16pt" class="svg-formula" dspmath="mathimg" md5hash="1467477ecea38809b6b6f06c82d8832a"><svg:image xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="mr-2-447-2021-ie00002.svg" width="27pt" height="16pt" src="mr-2-447-2021-ie00002.png"/></svg:svg></span></span>(180<span class="inline-formula"><sub>0</sub></span>) or <span class="inline-formula"><math xmlns="http://www.w3.org/1998/Math/MathML" id="M22" display="inline" overflow="scroll" dspmath="mathml"><mrow><mi mathvariant="normal">R</mi><msubsup><mn mathvariant="normal">16</mn><mn mathvariant="normal">7</mn><mn mathvariant="normal">6</mn></msubsup></mrow></math><span><svg:svg xmlns:svg="http://www.w3.org/2000/svg" width="27pt" height="16pt" class="svg-formula" dspmath="mathimg" md5hash="77936c715f231774d5e767150eec791c"><svg:image xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="mr-2-447-2021-ie00003.svg" width="27pt" height="16pt" src="mr-2-447-2021-ie00003.png"/></svg:svg></span></span>(270<span class="inline-formula"><sub>0</sub></span>90<span class="inline-formula"><sub>180</sub></span>) schemes at <span class="inline-formula"><i>ν</i><sub>R</sub>=20</span> or 62.5âkHz, respectively. The <span class="inline-formula"><i>D</i></span>-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 <span class="inline-formula"><i>ν</i><sub>R</sub>=62.5</span>âkHz to acquire in 72âmin 2D HETCOR (heteronuclear correlation) spectra between <span class="inline-formula"><sup>1</sup></span>H and quadrupolar nuclei, with a non-uniform sampling (NUS).
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