Polarization losses from the nonadiabatic passage of hyperpolarized solutions through metallic components

James Eills , Marc Azagra , David Gómez-Cabeza , Michael C.D. Tayler , Irene Marco-Rius
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Abstract

From complex-mixture analysis to in vivo molecular imaging, applications of liquid-state nuclear spin hyperpolarization have expanded widely over recent years. In most cases, hyperpolarized solutions are generated ex situ and transported from the polarization instrument to the measurement device. The sample hyperpolarization usually survives this transport, since the changes in magnetic fields that are external to the sample are typically adiabatic (slow) with respect to the internal nuclear spin dynamics. The passage of polarized samples through weakly magnetic components such as stainless steel syringe needles and ferrules is not always adiabatic, which can lead to near-complete destruction of the magnetization. To avoid this effect becoming “folklore” in the field of hyperpolarized NMR, we present a systematic investigation to highlight the problem and investigate possible solutions. Experiments were carried out on: (i) dissolution-DNP-polarized [1-13C]pyruvate with NMR detection at 1.4 T, and (ii) 1.5-T-polarized H2O with NMR detection at 2.5 μT. We show that the degree of adiabaticity of solutions passing through metal parts is intrinsically unpredictable, likely depending on many factors such as solution flow rate, degree of remanent ferromagnetism in the metal, and nuclear spin species. However, the magnetization destruction effects can be suppressed by application of an external field on the order of 0.1–10 mT.

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超极化溶液通过金属元件时产生的非绝热极化损耗
从复杂混合物分析到体内分子成像,液态核自旋超极化的应用近年来得到了广泛拓展。在大多数情况下,超极化溶液是在原位生成的,并从极化仪器传输到测量装置。由于相对于内部核自旋动态而言,样品外部磁场的变化通常是绝热的(缓慢的),因此样品的超极化通常能在传输过程中存活下来。极化样品通过弱磁性部件(如不锈钢注射针头和卡套)时并不总是绝热的,这会导致磁化几乎完全破坏。为了避免这种效应成为超极化 NMR 领域的 "民间传说",我们开展了一项系统调查,以突出这一问题并研究可能的解决方案。实验的对象是:(i) 溶解-DNP 极化[1-13C]丙酮酸盐,在 1.4 T 下进行 NMR 检测;(ii) 1.5 T 极化 H2O,在 2.5 μT 下进行 NMR 检测。我们的研究表明,通过金属部件的溶液的绝热程度本质上是不可预测的,可能取决于许多因素,如溶液流速、金属中的剩磁铁磁性程度以及核自旋种类。不过,施加 0.1-10 mT 量级的外部磁场可以抑制磁化破坏效应。
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