2002
DOI: 10.1016/s0168-583x(02)01105-9
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The Coulomb explosion of molecular ions in channeling conditions

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Cited by 18 publications
(10 citation statements)
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“…The correct fitting between simulated and experimental data in the case of the atomic beams, Q ␣ Q ␤ = 0, also implies that the model used, which does not take into account any charge exchange process, is valid in the bulk region selected for the study, as proven also in Ref. 41. Evidently, the same value of A 0 was also used for all the molecular ion cases, Q ␣ Q ␤ 0, but in this case, Q ␣ Q ␤ was varied independently for all the possible combinations of the ionization states of the C 2 + molecule: from Q ␣ Q ␤ =1 to Q ␣ Q ␤ = 36.…”
Section: B Validation Of the Monte Carlo Simulationsmentioning
confidence: 74%
See 1 more Smart Citation
“…The correct fitting between simulated and experimental data in the case of the atomic beams, Q ␣ Q ␤ = 0, also implies that the model used, which does not take into account any charge exchange process, is valid in the bulk region selected for the study, as proven also in Ref. 41. Evidently, the same value of A 0 was also used for all the molecular ion cases, Q ␣ Q ␤ 0, but in this case, Q ␣ Q ␤ was varied independently for all the possible combinations of the ionization states of the C 2 + molecule: from Q ␣ Q ␤ =1 to Q ␣ Q ␤ = 36.…”
Section: B Validation Of the Monte Carlo Simulationsmentioning
confidence: 74%
“…41 To simulate the ion flux behavior in channeling and in random configuration for atomic ions, the Coulomb interaction was set to zero. Thus Q ␣ Q ␤ = 0, where Q is the charge of atom of a molecular ion.…”
Section: B Validation Of the Monte Carlo Simulationsmentioning
confidence: 99%
“…However, the computer simulations employed in such study strongly overestimated the experimental results. (Khodyrev et al, 2002).…”
Section: Introductionmentioning
confidence: 99%
“…More recently, new backscattering results interpreted in terms of computer simulations allowed a better understanding of the consequences due to the Coulomb explosion of molecules under channeling conditions. 7 Moreover, a refined experiment combining the detection of both x-rays and backscattered particles from crystal Si allowed a quantitative measure of the transversal Coulomb heating energy. 8 These results showed that this energy, for the cases of H 2 + and H 3 + traveling along the Si͗100͘ channel at 150 kev/ amu, amounts to 2.6± 0.6 eV and 5.1± 0.8 eV respectively, which are compatible with the potential energy stored per particle in the molecule.…”
Section: Introductionmentioning
confidence: 99%