聚类和异质P1分布在6.9和13.8T的钻石 DNP机制
Orit Nir-Arad1, David H Shlomi1, Raj K Chaklashiya2,3
1School of Chemistry, Faculty of Exact Sciences, Tel Aviv University, Tel Aviv 6997801, Israel.
The journal of physical chemistry letters
|October 13, 2025
概括
钻石中的P1中心能够实现显著的C超极化. 在高电场下,P1集群对于高效的动态核极化 (DNP) 是必不可少的,允许绘制钻石缺陷的地图.
科学领域:
- 固态物理 固态物理
- 量子信息科学是一种量子信息科学.
- 材料科学是一种材料科学.
背景情况:
- 钻石中的替代 (P1中心) 对于13C超极化至关重要.
- P1集群在动态核极化 (DNP) 效率中的作用仍在调查中.
研究的目的:
- 为了调查P1集群对于单晶钻石中高场C DNP的必要性.
- 区分固体效应 (SE) 和交叉效应 (CE) DNP机制.
- 探索DNP在空间绘制钻石缺陷方面的能力.
主要方法:
- 在6.9和13.8 T的C DNP和电子磁共振 (EPR) 光谱的比较.
- 分析高 (∼20 ppm) 和低 (∼3.5 ppm) P1 度的钻石,有或没有P1 集群.
- 测量13C极化积累率作为毫米波频率的函数.
主要成果:
- 具有高P1度和集群的钻石显示出显著的C NMR增强 (540 ± 180 nm),具有宽窄的DNP特征.
- 低P1度和没有集群的钻石只表现出弱弱的,尖的DNP峰值.
- 极化积累的频率依赖证实P1集群对于高效的高场DNP (SE与CE) 是必不可少的.
结论:
- 在钻石中,P1集群对于高效的高场C DNP是不可或缺的.
- 高P1度钻石中的SE和CE机制使不同的C核池两极化.
- 动态核极化可以有效地绘制出钻石缺陷的空间分布.
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