International
Tables for
Crystallography
Volume C
Mathematical, physical and chemical tables
Edited by E. Prince

International Tables for Crystallography (2006). Vol. C. ch. 4.2, pp. 195-196

Section 4.2.1.4. Radioactive X-ray sources

U. W. Arndta

4.2.1.4. Radioactive X-ray sources

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Radioactive sources of X-rays are mainly of interest to crystallographers for the calibration of X-ray detectors where they have the great advantage of being completely stable with time, or at least of having an accurately known decay rate. For some purposes, spectral purity of the radiation is important; radionuclides that decay wholly by electron capture are particularly useful as they produce little or no β or other radiation. In this type of decay, the atomic number of the daughter nucleus is one less than that of the decaying isotope, and the emitted X-rays are characteristic of the daughter nucleus. In some cases, the probability of electron capture taking place from some shell other than the K shell is very small and most of the photons emitted are K photons. The number of photons emitted into a solid angle of 4π, uncorrected for absorption, is given by the strength of the source in Curies (1 Curie = 3.7 × 1010 disintegrations s−1), since each disintegration produces one photon. A list of these nuclei (after Dyson, 1973[link]) is given in Table 4.2.1.5[link].

Table 4.2.1.5| top | pdf |
Radionuclides decaying wholly by electron capture, and yielding little or no γ-radiation

NuclideHalf-lifeX-raysRemarks
Element[K{\alpha_1}] (keV)
37Ar35 dCl2.622
51Cr 27.8 dV4.952γ at 320 keV
55Fe2.6 aMn5.898
71Ge11.4 dGa9.251
103Pd17 dRh20.214Several γ's; all weak
109Cd453 dAg22.16γ at 88 keV
125I60 dTe27.47γ at 35.4 keV
131Cs10 dXe29.80
145Pm17.7 aNd37.36γ's at 67 and 72 keV
145Sm340 dPm38.65γ's at 61 keV; weak γ at 485 keV
179Ta600 dHf55.76
181W140 dTa57.52γ at 6.5 keV; weak γ's at 136, 153 keV
205Pb5 × 107 aTlL only (Lα1 = 10.27 keV)

Useful radioactive sources are also made by mixing a pure β-emitter with a target material. These sources produce a continuous spectrum in addition to the characteristic line spectrum. The nuclide most commonly used for this purpose is tritium which emits β particles with an energy up to 18 keV and which has a half-life of 12.4 a.

Radioactive X-ray sources have been reviewed by Dyson (1973[link]).

References

First citation Dyson, N. A. (1973). X-rays in atomic and nuclear physics. London: Longman.Google Scholar








































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