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核磁共振中的广义磁化到单重态序转移

Generalised magnetisation-to-singlet-order transfer in nuclear magnetic resonance.

作者信息

Bengs Christian, Sabba Mohamed, Jerschow Alexej, Levitt Malcolm H

机构信息

School of Chemistry, University of Southampton, University Road, SO17 1BJ, UK.

Department of Chemistry, New York University, New York, NY 10003, USA.

出版信息

Phys Chem Chem Phys. 2020 May 6;22(17):9703-9712. doi: 10.1039/d0cp00935k.

Abstract

A variety of pulse sequences have been described for converting nuclear spin magnetisation into long-lived singlet order for nuclear spin-1/2 pairs. Existing sequences operate well in two extreme parameter regimes. The magnetisation-to-singlet (M2S) pulse sequence performs a robust conversion of nuclear spin magnetisation into singlet order in the near-equivalent limit, meaning that the difference in chemical shift frequencies of the two spins is much smaller than the spin-spin coupling. Other pulse sequences operate in the strong-inequivalence regime, where the shift difference is much larger than the spin-spin coupling. However both sets of pulse sequences fail in the intermediate regime, where the chemical shift difference and the spin-spin coupling are roughly equal in magnitude. We describe a generalised version of M2S, called gM2S, which achieves robust singlet order excitation for spin systems ranging from the near-equivalence limit well into the intermediate regime. This closes an important gap left by existing pulse sequences. The efficiency of the gM2S sequence is demonstrated numerically and experimentally for near-equivalent and intermediate-regime cases.

摘要

已经描述了多种用于将核自旋磁化转换为核自旋 1/2 对的长寿命单重态序的脉冲序列。现有序列在两个极端参数范围内运行良好。磁化到单重态(M2S)脉冲序列在近等效极限下能将核自旋磁化稳健地转换为单重态序,这意味着两个自旋的化学位移频率之差远小于自旋 - 自旋耦合。其他脉冲序列在强不等效区域运行,其中位移差远大于自旋 - 自旋耦合。然而,这两组脉冲序列在中间区域都失效,在该区域化学位移差和自旋 - 自旋耦合的大小大致相等。我们描述了一种广义的 M2S,称为 gM2S,它对于从近等效极限到中间区域的自旋系统都能实现稳健的单重态序激发。这填补了现有脉冲序列留下的一个重要空白。gM2S 序列的效率在数值上和实验上都针对近等效和中间区域的情况进行了验证。

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