2004
DOI: 10.1103/physreva.70.032712
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Electron loss from1.4MeVuU4,6,10+ions colliding with Ne,et al.

Abstract: Absolute, total, single-and multiple-electron-loss cross sections are measured for 1.4-MeV/ u U 4,6,10+ ions colliding with neon and argon atoms and nitrogen molecules. It is found that the cross sections all have the same dependence on the number of electrons lost and that multiplying the cross sections by the initial number of electrons in the 6s, 6p, and 5f shells yields good agreement between the different projectiles. By combining the present data with previous measurements made at the same velocity, it i… Show more

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Cited by 41 publications
(20 citation statements)
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“…The production rate has been set to 10 13 ions per second which is a factor of 10 above the present estimates for the EURISOL facility.…”
Section: Discussionmentioning
confidence: 99%
See 1 more Smart Citation
“…The production rate has been set to 10 13 ions per second which is a factor of 10 above the present estimates for the EURISOL facility.…”
Section: Discussionmentioning
confidence: 99%
“…GSI for the future FAIR facility [10] and at BNL for the RHIC program. Experience from the Experimental Storage Ring (ESR) at GSI [14] suggests that it it is possible to keep recombination and stripping losses low.…”
Section: Acceleration and Storage Of Partly Charged Ionsmentioning
confidence: 99%
“…In contrast to the electron and proton ionization cross-sections, where experimental data or theoretical calculations exist for practically any ion or atom, the knowledge of ionization cross-sections by fast complex ions and atoms is far from complete. For this reason the US Heavy Ion Fusion Science Virtual National Laboratory has initiated measurements of cross-sections in a series of experiments at GSI [11][12][13] and the Texas A&M synchrotron [14,15]. When experimental data and theoretical calculations are not available, approximate formulae are needed; therefore, the scaling of cross-sections with energy and target or projectile nucleus charge has been developed to approximate these values of cross-sections over a broad range of energies and charge states [1,12,16].…”
Section: Introductionmentioning
confidence: 98%
“…To benchmark the theoretical approaches and semiempirical scaling laws developed for such systems, experimental data covering a wide range of collision energies as well as ion species and target systems are needed. Previous experimental studies of the EL cross sections of low-charged, heavy ions were mainly restricted to energies below 10 MeV=u [20][21][22][23][24][25][26][27][28][29][30], whereas for ion-driven fusion scenarios beam energies ranging from about 15 MeV=u up to roughly 500 MeV=u [31] are most relevant and in case of the FAIR facility the energy region of interest even extends up to the relativistic GeV=u regime. Recently, we presented a first EL cross section measurement for a low-charged ion, namely U 28þ , covering beam energies up to 50 MeV=u that was performed at the experimental storage ring (ESR) of the GSI Helmholtz Center for Heavy Ion Research [32].…”
Section: Introductionmentioning
confidence: 99%