Gamma Radioactivity伽马放射性
Gamma radiation is the most useful type of radiation for medical purposes, but at the same time it is the most dangerous because of its ability to penetrate large thicknesses of material. 伽马射线是用于医疗目的最有用的辐射类型,但同时它也是最危险的,因为其能穿透大量材料的能力。 |
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Other Radioactive Processes其他放射性过程
While the most common types of radioactive decay are by alpha, beta, and gamma radiation, several other varieties of radioactivity occur: 尽管最常见的放射性衰变方式是通过α、β和γ射线,但还有几种其他形式的放射性现象发生:
Electron capture: A parent nucleus may capture one of its own electrons and emit a neutrino. This is exhibited in the potassium-argon decay. 电子捕获:母核可能捕获其自身的其中一个电子并发射一个中微子。这种现象在钾-氩衰变中有所体现。
Positron or positive beta decay: Positron emission is called beta decay because the characteristics of electron or positron decay are similar. They both show a characteristic energy spectrum because of the emission of a neutrino or antineutrino. 正电子或正β衰变:正电子发射被称为β衰变,因为电子或正电子衰变的特性相似。它们都显示出特征的能量谱,因为发射了中微子或反中微子。
Internal conversion is the use of electromagnetic energy from the nucleus to expel an orbital electron from the atom. 内转换是利用原子核的电磁能将轨道电子从原子中射出。
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Electron Capture电子捕获
The capture of the electron by a proton in the nucleus is accompanied by the emission of a neutrino. The process leaves a vacancy in the electron energy level from which the electron came, and that vacancy is either filled by the dropping down of a higher-level electron with the emission of an X-ray or by the ejection of an outer electron in a process called the Auger effect. ![]()
In the middle range of the periodic table, those isotopes which are lighter than the most stable isotopes tend to decay by electron capture, and those heavier decay by negative beta decay. An example of this pattern is seen with silver isotopes, with two stable isotopes plus one of lower mass which decays by electron capture and one of heavier mass which decays by beta emission. 在元素周期表的中间区域,那些比最稳定的同位素更轻的同位素倾向于通过电子捕获衰变,而更重的则通过负β衰变衰变。这种模式在银的同位素中可以见到,其中有两个稳定的同位素,一个质量较低的同位素通过电子捕获衰变,另一个质量较高的同位素通过β衰变衰变。
质子在核内捕获一个电子的过程中,会伴随中微子的发射。该过程会在电子原来能量水平上留下一个空位,这个空位要么由一个较高能级的电子跃迁到该水平并发射X射线来填补,要么通过外层电子的电离来填补,这种现象称为Auger效应。 An important example of electron capture decay is that of potassium-40 since it forms the basis for the potassium-argon mineral dating process. ![]()
电子捕获衰变的一个重要例子是钾-40,因为它构成了钾-氩矿物测年过程的基础。
一个典型例子是铍-7的衰变:⁴Be → ⁷Li + ⁰₋₁e + ν |
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Internal Conversion内部转换
Internal conversion is another electromagnetic process which can occur in the nucleus and which competes with gamma emission. Sometimes the multipole electric fields of the nucleus interact with orbital electrons with enough energy to eject them from the atom. This process is not the same as emitting a gamma ray which knocks an electron out of the atom. It is also not the same as beta decay, since the emitted electron was previously one of the orbital electrons, whereas the electron in beta decay is produced by the decay of a neutron. 内转换是另一种核内的电磁过程,它与伽马射线发射竞争。有时,核的多极电场与轨道电子相互作用,如果能量足够,可以将它们从原子中击出。这个过程并不是像发射伽马射线那样将电子击出原子,也不是像β衰变那样,因为发射的电子原本就是轨道电子,而β衰变中的电子是由中子衰变产生的。
![]() An example used by Krane is that of 203Hg, which decays to 203Tl by beta emission, leaving the 203Tl in an electromagnetically excited state. It can proceed to the ground state by emitting a 279.190 keV gamma ray, or by internal conversion. In this case the internal conversion is more probable. Since the internal conversion process can interact with any of the orbital electrons, the result is a spectrum of internal conversion electrons which will be seen as superimposed upon the electron energy spectrum of the beta emission. The energy yield of this electromagnetic transition can be taken as 279.190 keV, so the ejected electrons will have that energy minus their binding energy in the 203Tl daughter atom. Krane举了一个例子,即203Hg衰变到203Tl,通过β衰变,使203Tl处于电磁激发态。它可以通过发射279.190 keV的伽马射线或内转换跃迁到基态。在这种情况下,内转换更为 probable。由于内转换过程可以与任何轨道电子相互作用,结果是一系列内转换电子的能量谱,这将叠加在β衰变的电子能量谱上。这个电磁跃迁的能量可以取为279.190 keV,因此被击出的电子将具有该能量减去其在203Tl子原子中的结合能。
The diagram above is of course conceptual only and not to scale since the nuclear radius of thallium is modeled to be about 0.7x10-14 m and the radius of the atom is about 1.76x10-10m, a factor of about 25,000 larger! And of course the planetary type orbits of the electrons are unrealistic since the wave properties of the electrons lead to charge distributions that give a finite probability that the K electron shown above will actually extend inside the nucleus so that the nucleus can interact with it and hand off its excess energy. An examination of the electron distribution for the simplest atom, hydrogen, can give the perspective that the electron has a small but finite probability of extending into the nucleus. From the table of binding energies below, you can see that the binding energy of the K-shell electron is over 85,000 electron volts compared to 13.6 eV for the hydrogen electron, or over 6,000 times larger.
The resolution of the electron detection is good enough that such internal conversion electron spectra can be used to study the binding energies of the electrons in heavy atoms. In this case, the measured electron energies can be subtracted from the transition energy as indicated by the gamma emission, 279.190 keV. 电子探测的分辨率足够高,使得这类内部转换电子谱可以用来研究重原子中电子的结合能。在这种情况下,测得的电子能量可以从伽马射线发射所指示的跃迁能量279.190 keV中减去。
In addition to information from the internal conversion electrons about the binding energies of the electrons in the daughter atom, the relative intensities of these internal conversion electron peaks can give information about the electric multipole character of the nucleus. 除了来自内部转换电子的关于子核中电子结合能的信息外,这些内部转换电子峰的相对强度还能提供关于核的电四极子特征的信息。
上面的图当然是概念性的,而且不按比例绘制,因为铊的核半径被建模为约0.7×10⁻¹⁴ m,而原子的半径约为1.76×10⁻¹⁰ m,大约大25,000倍!当然,电子的行星型轨道是不现实的,因为电子的波性质导致电荷分布,使得上面所示的K电子实际上有有限的概率延伸到核内,从而使核能够与它相互作用并传递其多余能量。对最简单的原子氢的电子分布进行考察,可以得到电子有很小但有限的概率延伸到核内的观点。从下面的结合能表中,你可以看到K壳层电子的结合能超过85,000电子伏,相比之下,氢原子电子的结合能仅为13.6 eV,或大约6,000倍。 |
Index Reference Krane Nuclear Physics, Sec 10.6 Internal conversion Wiki 索引参考 Krane 核物理,第 10 章 6 节 内转换 Wiki | ||||||||||||||||||||
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Discovery of Radioactivity放射性发现
Radioactivity was discovered by A. H. Becquerel in 1896. The radiation was classified by E. Rutherford as alpha, beta, and gamma rays according to their ability to penetrate matter and ionize air. 放射性是由A. H. 贝克勒尔于1896年发现的。E. 伦琴根据辐射穿透物质和电离空气的能力将其分类为α、β和γ射线。
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