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Energy and Momentum Spectra for Beta Decay

β衰变的能谱与动量谱

Beta emission has a characteristic energy spectrum. It is accompanied by the emission of an electron antineutrino which shares the momentum and energy of the decay.

β衰变具有特征的能量谱。它伴随着一个电子和反中微子的发射,后者分享衰变的动量和能量。

This experimental energy spectrum is from G. J. Neary, Roy. Phys. Soc. (London), A175, 71 (1940).

这个实验能量谱来自G. J. Neary,刊载于《皇家物理学会会刊》(伦敦),A175,71(1940)。

From the Fermi theory of beta decay, the shape of the energy distribution for this "allowed" transition is given approximately by the expression

根据费米对β衰变的理论,这种‘允许’跃迁的能量分布近似由下式给出

where F(Z',KEe) is called the Fermi function. It accounts for the nuclear coulomb interaction which shifts this distribution toward lower energies because of the coulomb attraction between the daughter nucleus and the emitted electron. (It shifts the distribution upward for positrons.) Q represents the energy yield of the transition and as such is the upper bound on the kinetic energy of the electron, KEe. The apparent complexity of the expression is partly because it is necessary to use relativistic momentum for the electron.

其中F(Z',KE e )被称为费米函数。它考虑了核库仑相互作用,由于子核与发射出的电子之间的库仑吸引力,使这一分布向更低的能量偏移。(对于正电子来说,它会使分布向上偏移。)Q表示该转变的能量产出,因此是电子动能KE e 的上限。表达式看似复杂,部分原因是必须使用相对论性动量来描述电子。
The emission of the electron's antiparticle, the positron, is also called beta decay.
电子的反粒子——正电子的发射,也称为β衰变。

The nucleus 64Cu is a good example for momentum spectra since it decays by both electron (to 64Zn) and positron emission (to 64Ni) with comparable transition energies. The experimental spectra below are from Cook and Langer, Phys. Rev. 73, 601 (1948) with theoretical refinement by J. R. Reitz, Phys. Rev. 77, 10 (1950). This allows you to see clearly that the momentum spectrum of the positron is shifted toward higher momentum by the coulomb repulsion of the nucleus.

铜-64核是动量谱的良好例子,因为它通过电子发射(转变为锌-64)和正电子发射(转变为镍-64)衰变,两种衰变过程的跃迁能量相当。下面的实验谱来自Cook和Langer,Phys. Rev. 73, 601 (1948),并由J. R. Reitz进行理论修正,Phys. Rev. 77, 10 (1950)。这使你能够清楚地看到正电子的动量谱因库仑斥力而向更高动量方向偏移。

From the Fermi theory of beta decay, the shape of the distributions for these "allowed" transitions is given approximately by the expression

根据费米对β衰变的理论,这些‘允许’跃迁的分布形状近似由下式给出

where F(Z',p) is called the Fermi function. It accounts for the nuclear coulomb interaction and is the main source of the difference between the two curves above. Again, the expression looks a bit complex because the relativistic relationship between momentum and enegy must be used for beta decay.

其中F(Z',p)被称为费米函数。它考虑了核库仑相互作用,并是上述两条曲线差异的主要来源。再次,这个表达式看起来有点复杂,因为β衰变必须使用动量与能量的相对关系。
Index

Beta decay concepts

Reference
Cohen
Concepts of Nuclear Physics, Sec 11-1
索引 β衰变概念 参考 Cohen 核物理概念,第11-1节
 
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