1974
DOI: 10.1103/physreva.10.1230
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Zdependence ofK αx-ray satellite structure in heavy-ion—atom collisions

Abstract: The spectra of Ka x rays emitted as a result of heavy-ionatom collisions have been measured with a Bragg spectrometer using a variety of equal velocity (1.7 MeV/amu) heavy ions ranging from, H to , SAr incident on solid targets containing atoms of »Al, »Cl, and»K. In the cases of Cl and K, the measured Kal, -Ka satellite energy differences for one through seven L-shell vacancies were found to be systematically larger than those calculated using the Herman-SkillmanHartree-Fock-Slater program.Values of the binom… Show more

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Cited by 76 publications
(12 citation statements)
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“…The spectra (see Fig. The energies of the satellite peaks are consistent with Hartree-Fock-Slater calculations for multiply ionized atoms (Burkhalter et al, 1972;Watson et al, 1974). In this particular case, the first peak is composed of the usual Kal and Ka2 diagram lines whereas the peaks which follow are satellite peaks composed of Κα χ rays arising from configurations having n (one, two, .…”
Section: B Satellite Peakssupporting
confidence: 73%
See 1 more Smart Citation
“…The spectra (see Fig. The energies of the satellite peaks are consistent with Hartree-Fock-Slater calculations for multiply ionized atoms (Burkhalter et al, 1972;Watson et al, 1974). In this particular case, the first peak is composed of the usual Kal and Ka2 diagram lines whereas the peaks which follow are satellite peaks composed of Κα χ rays arising from configurations having n (one, two, .…”
Section: B Satellite Peakssupporting
confidence: 73%
“…The binomial probability parameter pL may be interpreted approximately as the average L-shell ionization probability per electron for K-shell ioniz ing collisions (Watson et al, 1974). The/?L values (and the absolute cross sections for satellite production) can be calculated from theory (Kauffman et al, 1973;McGuire and Richard, 1973) but the agreement between experiment and theory is generally poor.…”
Section: B Satellite Peaksmentioning
confidence: 99%
“…It was reported [2,3] that satellite yields for low Z elements were well reproduced by the binomial distribution. There may be two reasons for the apparent difference with the present case: to begin with the data of [-2, 3] were obtained for lower beam energies ( < 2 Mev/u) where the K-shell of the projectile is partly occupied, thus decreasing the importance of the L ~ K capture process (capture to L, M...-shells produces vacancy distributions similar to the binomial one with n = 8).…”
Section: P~c(ol)=(1--pc)(l-1)/2(l--pc)(l+l)/2=(1--pc)zmentioning
confidence: 85%
“…From the literature we have found that the closest line is the Ly-β line of H-like Sc, and the next nearest line is the Ly-α line of Ti (see Table 5, Deslattes et al 2003, and references therein). It is still possible that the line is the He-like Sc line shifted to higher energy if the line has been produced in ion-atom collisions and has a few satellites (Watson et al 1974). Depending on the line identification one can consider different production mechanisms.…”
Section: +018mentioning
confidence: 99%