Resonant Mixing Dynamic Nuclear Polarization

被引:3
|
作者
Quan, Yifan [1 ,2 ]
Ouyang, Yifu [1 ,2 ]
Mardini, Michael [1 ,2 ]
Palani, Ravi Shankar [1 ,2 ]
Banks, Daniel [3 ]
Kempf, James [3 ]
Wenckebach, W. Tom [4 ,5 ]
Griffin, Robert G. G. [1 ,2 ]
机构
[1] MIT, Francis Bitter Magnet Lab, Cambridge, MA 02139 USA
[2] MIT, Dept Chem, Cambridge, MA 02139 USA
[3] Bruker Biospin, Billerica, MA 01821 USA
[4] Paul Scherrer Inst, CH-5232 Villigen, Switzerland
[5] Univ Florida, Natl High Magnet Field Lab, Gainesville, FL 32310 USA
来源
JOURNAL OF PHYSICAL CHEMISTRY LETTERS | 2023年 / 14卷 / 31期
基金
美国国家卫生研究院; 瑞士国家科学基金会;
关键词
Coupled spins - Cross effects - Density matrix - Dynamic nuclear polarization - Microwave field - Mixing dynamics - Overhauser effect - Simple++ - Solid effects - Thermal mixing process;
D O I
10.1021/acs.jpclett.3c01869
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
We propose a mechanism for dynamic nuclear polarizationthat isdifferent from the well-known Overhauser effect, solid effect, crosseffect, and thermal mixing processes. We term it ResonantMixing (RM), and we show that it arises from the evolutionof the density matrix for a simple electron-nucleus coupledspin pair subject to weak microwave irradiation, the same interactionsas the solid effect. However, the SE is optimal when the microwavefield is off-resonance, whereas RM is optimal when the microwave fieldis on-resonance and involves the mixing of states by the microwavefield together with the electron-nuclear coupling. Finally,we argue that this mechanism is responsible for the observed dispersive-shapedDNP field profile for trityl samples near the electron paramagneticresonance center.
引用
收藏
页码:7007 / 7013
页数:7
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