Shan Liang
National Center for Biotechnology Information, NLM, NIH
Magnetic resonance spectroscopy (MRS) is a technique that allows us to non-invasively detect multiple small metabolites within cells or extracellular spaces (1-3). The clinical use of MRS as an adjunct to magnetic resonance imaging (MRI), particularly in cancer detection and treatment response evaluation, has expanded dramatically over the past several years. Although MRS is theoretically applicable to any nucleus possessing spin, the most important and more frequently investigated applications are in proton (H) and carbon-13 (C) (4-6). C MRS is superior to H MRS in many respects (3, 6-8). C MRS can provide specific information about the identity and structure of biologically important compounds. The chemical shift range for carbon (250 ppm) is much larger than that for proton (15 ppm), allowing for improved resolution of metabolites. In addition, the T relaxation time of C in small molecules is much longer than that of H (0.1–2.0 s in a magnetic field of 0.1–3.0 T), allowing the generation of hyperpolarized C-labeled tracers outside the subject and the MRI scanner. Some of these tracers are endogenous and therefore have lower toxicity than drugs and exogenous contrast media (6). However, C MRS is limited by the low natural abundance of C (1.1%) and its low magnetogyric ratio (γ of C is one quarter that of H) (2, 3). Several techniques have been used to overcome the C MRS limitation through enhancing the polarization of nuclear spins. One technique is proton decoupling, which eliminates the coupling of H with C by irradiating the entire H resonance absorption range and consequently collapsing C resonances to singlets (4, 5). The signal/noise ratio of C resonances has been shown to be significantly increased with proton decoupling. Another technique is known as dynamic nuclear polarization (DNP), which introduces one or more C molecules into a metabolic substrate (2, 3, 8). DNP transfers high electron spin polarization to nuclear spins microwave irradiation. Nearly 100% nuclear polarization for H and 50% for C can be achieved in various organic molecules when DNP is performed in a strong magnetic field and at cryogenic temperatures. Replacing the C (98.9% natural abundance) isotope with the C isotope at a specific carbon or carbons in a metabolic substrate does not affect the substrate's biochemistry. With C MRS, the body tissues are virtually invisible, and only regions where the hyperpolarized C-labeled substance is present will appear in the generated images. Thus, C-labeled substrates can provide >10,000-fold enhancement of the C MRS signals from the substrate and its subsequent metabolic products, allowing the assessment of changes in metabolic fluxes through glycolysis, citric acid cycle, and fatty acid synthesis (1, 9-13). Vascular and perfusion imaging can also be performed without background signal from surrounding tissues (3, 14). Gallagher et al. generated a hyperpolarized small molecule, [1,4-C]fumarate, as an imaging agent of C MRS for evaluation of early tumor response to treatment and other pathological states in which cell death plays a role, such as toxic insults or ischemia (1). Fumarate, a tricarboxylic acid cycle intermediate, is hydrated to produce malate in a reaction catalyzed by fumarase (or fumarate hydratase). The transport of fumarate across the plasma membrane is mediated by the sodium-dependent dicarboxylate acid transporter, which also transports succinate. Fumarate transport across the mitochondrial membrane occurs in exchange for malate, inorganic phosphate, or aspartate. The reaction enzyme fumarase exists as both cytosolic and mitochondrial isoforms, and the relative activity of the two isoforms varies markedly between tissues and between species. The investigators showed that [1,4-C]malate production from [1,4-C]fumarate is increased in treated lymphoma cells and tumors, and that this increase is caused by tumor cell necrosis. The formation of hyperpolarized [1,4-C]malate from [1,4-C]fumarate appears to be a sensitive marker of tumor cell death and could be used to detect the early response of tumors to treatment (1).
磁共振波谱(MRS)是一种使我们能够无创检测细胞内或细胞外间隙中多种小分子代谢物的技术(1 - 3)。在过去几年中,MRS作为磁共振成像(MRI)的辅助手段在临床中的应用,尤其是在癌症检测和治疗反应评估方面,有了显著扩展。虽然从理论上讲,MRS适用于任何具有自旋的原子核,但最重要且研究更频繁的应用是针对质子(H)和碳 - 13(C)(4 - 6)。碳磁共振波谱(C MRS)在许多方面优于氢磁共振波谱(H MRS)(3,6 - 8)。C MRS能够提供有关生物重要化合物的身份和结构的特定信息。碳的化学位移范围(约250 ppm)比质子的化学位移范围(约15 ppm)大得多,这使得代谢物的分辨率得以提高。此外,小分子中碳的T弛豫时间比氢长得多(在0.1 - 3.0 T的磁场中为0.1 - 2.0 s),这使得能够在受试者体外和MRI扫描仪外生成超极化的碳标记示踪剂。其中一些示踪剂是内源性的,因此毒性比药物和外源性造影剂低(6)。然而,C MRS受到碳的天然丰度低(1.1%)及其低磁旋比(碳的γ是氢的四分之一)的限制(2,3)。已经使用了几种技术来通过增强核自旋的极化来克服C MRS的局限性。一种技术是质子去耦,通过照射整个氢共振吸收范围消除氢与碳的耦合,从而使碳共振坍缩为单峰(4,5)。已证明质子去耦可显著提高碳共振的信噪比。另一种技术称为动态核极化(DNP),它将一种或多种碳分子引入代谢底物中(2,3,8)。DNP通过微波辐射将高电子自旋极化转移到核自旋上。当在强磁场和低温下进行DNP时,在各种有机分子中可实现氢的近100%核极化和碳的50%核极化。在代谢底物的特定一个或多个碳原子处用碳同位素取代碳(98.9%天然丰度)同位素不会影响底物的生物化学性质。使用C MRS时,身体组织实际上是不可见的,只有存在超极化碳标记物质的区域才会出现在生成的图像中。因此,碳标记底物可使来自底物及其后续代谢产物的C MRS信号增强超过10000倍,从而能够评估通过糖酵解、柠檬酸循环和脂肪酸合成的代谢通量变化(1,9 - 13)。还可以在没有周围组织背景信号的情况下进行血管和灌注成像(3,14)。加拉格尔等人制备了一种超极化小分子[1,4 - C]富马酸盐,作为C MRS的成像剂,用于评估肿瘤对治疗的早期反应以及其他细胞死亡起作用的病理状态,如毒性损伤或缺血(1)。富马酸盐是三羧酸循环的中间体,在富马酸酶(或富马酸水合酶)催化的反应中被水合生成苹果酸。富马酸盐跨质膜的转运由钠依赖性二羧酸转运体介导,该转运体也转运琥珀酸盐。富马酸盐跨线粒体膜的转运以与苹果酸、无机磷酸或天冬氨酸交换的形式发生。反应酶富马酸酶以胞质和线粒体同工型存在,并且这两种同工型的相对活性在不同组织和不同物种之间有显著差异。研究人员表明,在经治疗的淋巴瘤细胞和肿瘤中,[1,4 - C]富马酸盐生成[1,4 - C]苹果酸的量增加,并且这种增加是由肿瘤细胞坏死引起的。由[1,4 - C]富马酸盐形成超极化的[1,4 - C]苹果酸似乎是肿瘤细胞死亡的敏感标志物,可用于检测肿瘤对治疗的早期反应(1)。