Technetium-99m锝-99m
Technetium-99m is a widely used radioactive tracer isotope in Nuclear Medicine. It's gamma ray energy of about 140 keV is convenient for detection. The fact that both its physical half-life and its biological half-life are very short leads to very fast clearing from the body after an imaging process. A further advantage is that the gamma is a single energy, not accompanied by beta emission, and that permits more precise alignment of imaging detectors. technetium-99m 是核医学中广泛使用的放射性示踪同位素。其伽马射线能量约为 140 keV,便于检测。其物理半衰期和生物半衰期都很短,导致在成像过程后从体内迅速清除。另一个优点是伽马射线是一种单一能量,不伴随β衰变,这使得成像探测器的对准更加精确。
Technetium -99m is produced by bombarding molybdenum 98Mo with neutrons. The resultant 99Mo decays with a half-life of 66 hours to the metastable state of Tc . This process permits the production of 99mTc for medical purposes. Since 99Mo is a fission product of 235U fission, it can be separated from the other fission products and used to generate 99mTc. For medical purposes, the 99mTc is used in the form of pertechnate, TcO4-. 技术尼姆-99m是通过用中子轰击钼-98Mo产生的。产生的99Mo衰变到技术尼姆的亚稳态,半衰期为66小时。这一过程使得可以生产用于医疗目的的99m Tc。由于99Mo是铀-235裂变产物,它可以与其他裂变产物分离并用于生成99m Tc。在医疗应用中,99m Tc以亚硝酸技术尼姆的形式使用,即TcO₄⁻。
The technetium isotope 99mTc is unusual in that it has a half-life for gamma emission of 6.03 hours. This is extremely long for an electromagnetic decay - more typical is 10-16 seconds. With such a long half-life for the excited state leading to this decay, this state is called a metastable state, and that is the reason for the designation 99m. Some aspects of the complex decay of this radioisotope are shown in the diagram below. The dominant decay mode gives the useful gamma ray at 140.5 keV. 99mTc的同位素具有一个特殊的性质,即其伽马射线的半衰期为6.03小时。这对于电磁衰变来说是非常长的——通常只有10-16秒。由于这种激发态的半衰期非常长,这个状态被称为亚稳态,这也是该同位素命名为99m的原因。下图展示了该放射性同位素复杂衰变的一些方面。主要的衰变方式会产生有用的伽马射线,能量为140.5 keV。
![]() While the 140.5 keV gamma transition is labeled as happening 98.6% of the time, not all of those actually emit a gamma ray photon. The process called internal conversion always competes with gamma photon emission. This involves transfer of the energy of the transition to one of the atomic electrons, usually a K, L, or M shell electron. This decay has been studied carefully enough to know the fraction of the decays associated with each pathway. 尽管140.5 keV的伽马跃迁被标记为98.6%的时间发生,但并非所有衰变都会发射伽马光子。这个过程称为内转换,总是与伽马光子发射竞争。这涉及将跃迁的能量转移到一个原子电子上,通常是一个K、L或M壳层电子。这种衰变已经被研究得足够详细,足以知道每种路径所关联的衰变分数。
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Index Nuclear applications to health Reference Hobbie Ch. 16 索引 核应用与健康 参考 Hobbie 第16章 | |||||||||||||||
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