Kreis Felix, Wright Alan J, Somai Vencel, Katz-Brull Rachel, Brindle Kevin M
Cancer Research UK Cambridge Institute, University of Cambridge, Cambridge, UK.
Department of Radiology, Faculty of Medicine, Hadassah Medical Center, Hebrew University of Jerusalem, Jerusalem, Israel.
Magn Reson Med. 2020 Oct;84(4):1844-1856. doi: 10.1002/mrm.28241. Epub 2020 Mar 10.
Hyperpolarized N-labeled molecules have been proposed as imaging agents for investigating tissue perfusion and pH. However, the sensitivity of direct N detection is limited by the isotope's low gyromagnetic ratio. Sensitivity can be increased by transferring N hyperpolarization to spin-coupled protons provided that there is not significant polarization loss during transfer. However, complete polarization transfer would limit the temporal window for imaging to the order of the proton T (2-3 s). To exploit the long T offered by storing polarization in N and the higher sensitivity of H detection, we have developed a pulse sequence for partial polarization transfer.
A polarization transfer pulse sequence was modified to allow partial polarization transfer, as is required for dynamic measurements, and that can be implemented with inhomogeneous B fields, as is often the case in vivo. The sequence was demonstrated with dynamic spectroscopy and imaging measurements with [ N ]urea.
When compared to direct N detection, the sequence increased the signal-to-noise ratio (SNR) by a factor of 1.72 ± 0.25, where both experiments depleted ~20% of the hyperpolarization (>10-fold when 100% of the hyperpolarization is used). Simulations with measured cross relaxation rates showed that this sequence gave up to a 50-fold increase in urea proton polarization when compared to spontaneous polarization transfer via cross relaxation.
The sequence gave an SNR increase that was close to the theoretical limit and can give a significant SNR benefit when compared to direct C detection of hyperpolarized [ C]urea.
超极化的氮标记分子已被提议作为用于研究组织灌注和pH值的成像剂。然而,直接检测氮的灵敏度受到该同位素低旋磁比的限制。如果在转移过程中没有明显的极化损失,通过将氮的超极化转移到自旋耦合的质子上,可以提高灵敏度。然而,完全极化转移会将成像的时间窗口限制在质子T2*的量级(2 - 3秒)。为了利用通过在氮中存储极化所提供的长T1以及氢检测的更高灵敏度,我们开发了一种用于部分极化转移的脉冲序列。
修改了极化转移脉冲序列,以允许进行动态测量所需的部分极化转移,并且该序列可以在不均匀的B场中实现,这在体内情况中经常出现。用[15N]尿素进行动态光谱和成像测量来演示该序列。
与直接检测氮相比,该序列将信噪比(SNR)提高了1.72 ± 0.25倍,其中两个实验都消耗了约20%的超极化(当使用100%的超极化时增加超过10倍)。用测量的交叉弛豫率进行的模拟表明,与通过交叉弛豫的自发极化转移相比,该序列使尿素质子极化增加了多达50倍。
该序列使SNR增加接近理论极限,并且与直接检测超极化的[13C]尿素的13C相比,可以带来显著的SNR优势。