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微波无 $^{13}$C 金刚石颗粒超极化:基于魔角旋转与NV色心

Microwave-Free $^{13}$C Hyperpolarization of Diamond Particles Enabled by Magic Angle Spinning and NV Centers

Rémi Blinder, Guzel Musabirova, Daehee Kim, Anshuman Nayak, Jason Twamley, Viateschlav N. Agafonov, Raiker Witter, Jörg Matysik, Fedor Jelezko

arXiv 2609.07653首次发表:更新:

发表机构

Okinawa Institute of Science and Technology Graduate University; University F. Rabelais(冲绳科学技术大学院大学; 弗朗索瓦·拉伯雷大学)

机构由 AI 辅助整理,请以论文原文为准。

AI 中文总结

本研究通过光泵浦NV色心结合魔角旋转,在无微波条件下实现金刚石颗粒中$^{13}$C核超极化,最高增强411倍,为室温高分辨率NMR铺路。

AI 中文摘要

固体中光泵浦色心产生的核超极化,为传统微波驱动的动态核极化(DNP)提供了一种替代方案。金刚石可容纳氮-空位(NV)色心,其基态自旋在室温下可通过光轻易极化,使金刚石成为核超极化的候选平台。我们报道了在随机取向的金刚石颗粒中,尺寸范围为0.2至2微米,在天然$^{13}$C丰度(1.1%)和20%同位素富集条件下,于7.1 T和9.4 T磁场下实现的$^{13}$C核超极化。该方案结合了光照明与魔角旋转(MAS),且无需微波辐照。通过在7.1 T磁场下,研究核极化随MAS频率(0至6 kHz)的变化,我们发现同位素富集样品的光诱导极化增强最大为280倍,天然丰度样品为411倍。在连续照明下,稳态绝对$^{13}$C极化水平超过0.1%。我们采用一个模型来描述这些发现,该模型涉及NV色心的光泵浦以及由NV、替代氮(P1)和$^{13}$C形成的三自旋簇中能级反交叉(LACs)附近的自旋动力学。该方案极大地减轻了NV自旋哈密顿量各向异性的影响,使得超过99.9%的NV取向能够参与极化转移过程。这些结果是将核极化从金刚石颗粒转移到外部核素的第一步,有望应用于室温下高灵敏度和高分辨率的核磁共振。

英文摘要

Nuclear hyperpolarization from optically pumped color centers in solids offers an alternative to conventional microwave-driven dynamic nuclear polarization (DNP). Diamond can host the nitrogen vacancy (NV) center, whose ground spin state can be readily polarized by light at room temperature, making diamond a candidate platform for nuclear hyperpolarization. We report $^{13}{\rm C}$ nuclear hyperpolarization in randomly oriented diamond particles with sizes ranging from 0.2 to 2 $μ$m, both at natural $^{13}{\rm C}$ abundance (1.1 %) and at 20 % isotopic enrichment, at magnetic fields of 7.1 T and 9.4 T. The protocol combines optical illumination with magic angle spinning (MAS) and does not require microwave irradiation. By investigating the nuclear polarization as a function of the MAS frequency between 0 and 6 kHz at the magnetic field of 7.1 T, we find maximum light-induced polarization enhancements of $280$-fold for the isotopically enriched sample and $411$-fold for the natural abundance sample. Under continuous illumination, steady-state absolute $^{13}{\rm C}$ polarization levels above 0.1 % are reached. A model involving optical pumping of NV centers and spin dynamics near level anticrossings (LACs) in three-spin clusters formed by NV, a substitutional nitrogen (P1) and $^{13}{\rm C}$ is used to describe these findings. The protocol strongly mitigates the effect of the anisotropy of the NV spin Hamiltonian, allowing more than $99.9\%$ of NV orientations to participate in the polarization transfer process. These results represent a first step toward transferring nuclear polarization from diamond particles to external nuclei, with potential applications in sensitive and high-resolution NMR at room temperature.

Comments64 pages (38 main text + 26 SI), 26 figures (9 main text + 17 SI), changed in v2: fixed figure references, complemented Funding and Acknowledgments

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