K-shell ionization cross sections for elements Se to Pd: 0.4 to 2.0 MeV

K-vacancy production by 3.6-, 4.75-, and 5.9-MeV/amu238U Ions

“…Counting rates were corrected by the ratio of the number of pulses triggered into the pre-amplifier to the number of pulses surviving in the pulser peak in the x-ray spectra. Cross sections were measured using the Rutherford monitoring technique [12]. A Si(Li) surface barrier detector, subtending a solid angle of ~10 .3 sterradians, was placed at a laboratory scattering angle of ~ 20 ~ The cross sections were checked by dividing the x-ray yields per projectile, measured by integrating the target current using the entire target chamber as a Faraday cup [7] by the target thickness.…”

MEASUREMENT OF THE CROSS SECTIONS FOR THE YIELD OF CHARACTERISTIC X-RAY RADIATION FROM 1-MeV PROTONS

“…546 [8] 446 [9] 446 [10] 478 [11] 667 [12] 478 [13] 605 [14] 480 [ Mo 0,27±0,02 0,049±0,010 0,32±0,02 0,23 [29] 0,29 [31] 0,22 [37] 0,218 [41] 0,23 [42] 0,239 [43] 0,23 [49] 0,22 [55] Ag 0,079±0,007 0,014±0,003 0,094±0,009 065 [15] 0,0706 [19] 0,078 [23] 0,0358 [30] 0,08 [32] 0,073 [36] 0,076 [37] 0,063 [42] 0,064 [44] 0,079 [45] 0,0618 [46] 0,087 [50] 0,067 [55] Cd 0,059±0,005 0,012±0,002 0,071±0,006 0,046 [39] 0,0346 [40] 0,049 [44] In 0,044±0,003 0,0082±0,0013 0,053±0,003 0,0612 [27] 0,036 [39] 0,0264 [40] 0,05 [45] 0,0377 [47] Sn 0,037±0,002 0,0068±0,0014 0,043±0,004 0,032 [15] 0,059 [31] 0,034 [37] 0,026 [39] 0,0167 [40] 0,029 [42] 0,037 [43] 0,032 [44] 0,051 [49] Sb 0,030±0,003 0,0064±0,0005 0,036±0,004 0,026 [15] 0,026 [44] 0,0257 [47] Т...…”