Magnetic Resonance Imaging磁共振成像
Proton nuclear magnetic resonance (NMR) detects the presence of hydrogens (protons) by subjecting them to a large magnetic field to partially polarize the nuclear spins, then exciting the spins with properly tuned radio frequency (RF) radiation, and then detecting weak radio frequency radiation from them as they "relax" from this magnetic interaction. The frequency of this proton "signal" is proportional to the magnetic field to which they are subjected during this relaxation process. In the medical application known as Magnetic Resonance Imaging (MRI), an image of a cross-section of tissue can be made by producing a well-calibrated magnetic field gradient across the tissue so that a certain value of magnetic field can be associated with a given location in the tissue. Since the proton signal frequency is proportional to that magnetic field, a given proton signal frequency can be assigned to a location in the tissue. This provides the information to map the tissue in terms of the protons present there. Since the proton density varies with the type of tissue, a certain amount of contrast is achieved to image the organs and other tissue variations in the subject tissue. 质子核磁共振(NMR)通过将氢原子(质子)置于强磁场中,使其核自旋部分极化,然后用适当调谐的射频(RF)辐射激发这些自旋,再检测它们在磁相互作用后“弛豫”时发出的微弱射频辐射,从而检测氢的存在。这种质子“信号”的频率与该弛豫过程中所受的磁场成正比。在称为磁共振成像(MRI)的医学应用中,可以通过在组织中产生良好的校准磁场梯度,使某一特定磁场值与组织中的特定位置相关联。由于质子信号频率与该磁场成正比,因此可以将某一质子信号频率分配给组织中的特定位置。这提供了将组织映射为其中所含质子的信息。由于质子密度随组织类型而变化,因此可以获得一定的对比度,以成像被检组织中的器官和其他组织变化。
The schematic below may help visualize the imaging process. It is presumed that there are two regions of the sample which contain enough hydrogens to produce a strong NMR signal. The top sketch visualizes an NMR process with a constant magnetic field applied to the entire sample. The hydrogen spin-flip frequency is then the same for all parts of the sample. Once excited by the RF signal, the hydrogens will tend to return to their lower state in a process called "relaxation" and will re-emit RF radiation at their Larmor frequency. This signal is detected as a function of time, and then is converted to signal strength as a function of frequency by means of a Fourier transformation. Since the protons in each of the active areas of the sample are subjected to the same magnetic field, they will produce the same frequency of radiation and the Fourier transform of the detected signal will have only one peak. This one peak demonstrates the presence of hydrogen atoms, but gives no information to locate them in the sample. 下面的示意图可能有助于可视化成像过程。假设样品中有两个区域含有足够的氢原子,能够产生强的核磁共振(NMR)信号。上图展示了在整个样品上施加恒定磁场的NMR过程。此时,氢原子的自旋翻转频率对于样品中的所有部分都是相同的。一旦被射频(RF)信号激发,氢原子将倾向于返回较低的能量状态,这一过程称为“弛豫”,并会在其拉莫尔频率下重新发射射频辐射。该信号随时间变化被检测,然后通过傅里叶变换将其转换为频率的信号强度。由于样品中每个活性区域的质子都处于相同的磁场中,它们将产生相同的辐射频率,因此检测到的信号的傅里叶变换将只有一个峰。这个单一的峰表明存在氢原子,但无法提供它们在样品中的具体位置信息。
![]() Information about the location of the hydrogen atoms can be obtained by adding a calibrated gradient field across the region of the sample as shown in the bottom sketch above. With an increasing magnetic field as you move to the right across the sample, the spin-flip energy and therefore the frequency of the emitted signal increases from left to right. When excited by an RF transmitter, the emitted signal contains different frequencies for the two proton concentration areas. These frequencies can be separated by means of the Fourier transform and the example gives two different regions of frequency for the two sample areas. This is the beginning of the process of locating the hydrogen atoms. In the sketch, it only locates them along the horizontal direction, giving no indication that they are at different heights. 通过在样品区域施加一个校准的梯度磁场(如上图下方的示意图所示),可以获得氢原子的位置信息。随着向右移动,磁场强度增加,因此自旋翻转的能级和由此产生的发射信号的频率从左到右逐渐增加。当由射频发射机激发时,发射的信号包含两个质子浓度区域的不同频率。这些频率可以通过傅里叶变换分离,示例中给出了两个不同频率区域对应样品的不同区域。这标志着定位氢原子过程的开始。在示意图中,它仅沿水平方向定位这些氢原子,没有表明它们位于不同的高度。
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Index Nuclear Spectra Concepts References Hobbie Ch 17 Bushong MRI 索引 核谱概念 参考文献 Hobie 第17章 Bushong MRI | |||||
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