1998
DOI: 10.1016/s0168-583x(98)80016-5
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Energy loss and straggling of H and He ions of keV energies in Si and C

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Cited by 97 publications
(34 citation statements)
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“…The method is based on collecting a series of spectra at different beam energies, and analysing them all simultaneously, with the continuous stopping power or cross section curve treated as fit parameters. For 4 He in Si, results equivalent within the experimental uncertainty to SRIM03 version 2006.02 [27] and Konac et al [28] were obtained [25].…”
Section: Advanced Algorithmsmentioning
confidence: 95%
“…The method is based on collecting a series of spectra at different beam energies, and analysing them all simultaneously, with the continuous stopping power or cross section curve treated as fit parameters. For 4 He in Si, results equivalent within the experimental uncertainty to SRIM03 version 2006.02 [27] and Konac et al [28] were obtained [25].…”
Section: Advanced Algorithmsmentioning
confidence: 95%
“…The inaccuracy of these stopping power values is cited to be 1-2%. [81], (the stopping cross-section used for this work), NKK96 = Niemann et al [82], SW80 = Santry and Werner [83], TRIM95 = Ziegler et al [75]) The accelerator used for RBS measurements was a National Electrostatics Corporation 3 MV tandem accelerator located at the Ion beam Materials Laboratory at Los Alamos National Laboratory, New Mexico, USA. The RBS spectra were obtained using a 4 He + beam with energies ranging from 2.0 MeV to 3.036 MeV.…”
Section: Mev Ion Beammentioning
confidence: 99%
“…For the incoming He ion beam, as in the RBS analysis, the stopping cross sections from Konac et al [81] were implemented in the computer program. The stopping power of the forward recoiled hydrogen atoms was also taken from the work of Konac et al (see figure [4][5][6][7][8] and implemented in the simulations, since their accuracy was shown to be 1-2% [88].…”
Section: Rbs Spectrummentioning
confidence: 99%
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