Charge states and energy loss of relativistic heavy ions in matter☆
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Cited by (36)
Accurate simultaneous lead stopping power and charge-state measurements in gases and solids: Benchmark data for basic atomic theory and nuclear applications
2023, Physics Letters, Section B: Nuclear, Elementary Particle and High-Energy PhysicsSimulation of angular and energy distributions for heavy evaporation residues using statistical model approximations and TRIM code
2013, Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated EquipmentCitation Excerpt :In the present work, the generation of the initial ER angular and energy distributions caused by neutron evaporation from a CN is considered in detail and compared with experimental data in Section 2. In Section 3, the suitability of the TRIM code [19] to the simulation of the angle and energy distributions for HI transmitted through solid targets is examined by the comparison of measured distributions available from literature with the simulated ones. In Section 4, some examples of the ER angular distributions resulted in simulations are compared with the corresponding ones obtained in experiments with thin targets.
MOCADI_FUSION: Extension of the Monte-Carlo code MOCADI to heavy-ion fusion-evaporation reactions
2008, Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and AtomsCitation Excerpt :The key ingredients of MOCADI_FUSION are: (i) the description of the nuclear interaction generating the ERs (see Section 2.1); (ii) the treatment of the atomic interaction of the ERs (see Section 2.2); (iii) the calculation of the separator ion optics (see Section 2.3). We used the statistical code PACE2 [17] to describe the nuclear reaction process leading to the production of the ERs, while the atomic interaction of the ERs with the target atoms can be treated either with ATIMA [18] or TRIM [19]. This procedure allows to define the phase-space of the ERs at the target exit via an event-by-event Monte-Carlo calculation.
Radiative electron capture in relativistic ion-atom collisions and the photoelectric effect in hydrogen-like high-Z systems
2007, Physics ReportsCitation Excerpt :At this final stage of beam handling, the electron cooler has to be switched on again. For the case of bare uranium ions the lowest beam energy achieved by this procedure is close to 5 MeV/u [60]. A further most important parameter of the target is its geometrical diameter of about 5 mm.
Wave packet approach to the ionization of high-Z, hydrogen-like ions
2003, Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and AtomsCitation Excerpt :Fig. 1 displays the total ionization cross-sections for fast Au78+ ions in collisions with thin carbon foils and as function of the projectile energy. In this figure, various theoretical cross-sections are compared with experiments from the GSI storage ring [14,15] and the measurements by Claytor et al. [16]. Following expression (2), either a ZT2 or ZT2+ZT scaling of the cross-sections for proton impact can be applied to obtain the total cross-sections.
Charge states of relativistic heavy ions in matter
1998, Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and Atoms