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基于液氢极化的质子磁共振成像。

Proton magnetic resonance imaging with para-hydrogen induced polarization.

机构信息

Max Planck Institute for Polymer Research, Ackermannweg 10, 55128 Mainz, Germany.

出版信息

Phys Chem Chem Phys. 2012 Feb 21;14(7):2346-52. doi: 10.1039/c2cp22822j. Epub 2012 Jan 12.

Abstract

A major challenge in imaging is the detection of small amounts of molecules of interest. In the case of magnetic resonance imaging (MRI) their signals are typically concealed by the large background signal of e.g. the body. This problem can be tackled by hyperpolarization which increases the NMR signals up to several orders of magnitude. However, this strategy is limited for (1)H, the most widely used nucleus in NMR and MRI, because the enormous number of protons in the body screens the small amount of hyperpolarized ones. Here, we describe a method giving rise to high (1)H MRI contrast for hyperpolarized molecules against a large background signal. The contrast is based on the J-coupling induced rephasing of the NMR signal of molecules hyperpolarized via PHIP and it can easily be implemented in common pulse sequences. We discuss several scenarios with different or equal dephasing times T(2)* for the hyperpolarized and thermally polarized compounds and verify our approach by experiments. This method may open up unprecedented opportunities to use the standard MRI nucleus (1)H for e.g. metabolic imaging in the future.

摘要

成像面临的一个主要挑战是检测到少量感兴趣的分子。在磁共振成像(MRI)的情况下,它们的信号通常被例如身体的大背景信号所掩盖。这个问题可以通过超极化来解决,超极化可以将 NMR 信号提高几个数量级。然而,这种策略对于(1)H 是有限制的,(1)H 是 NMR 和 MRI 中最广泛使用的核,因为体内大量的质子屏蔽了少量的超极化质子。在这里,我们描述了一种针对高极化分子的高对比度 MRI 方法,针对的是大背景信号。对比度基于通过 PHIP 超极化的分子的 J 耦合诱导的重新相位,它可以很容易地在常见的脉冲序列中实现。我们讨论了不同或相等的退相时间 T(2)*对于超极化和热极化化合物的几种情况,并通过实验验证了我们的方法。这种方法可能为将来使用标准 MRI 核(1)H 进行代谢成像等开辟前所未有的机会。

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