WebJun 5, 1993 · Recent results of stopping power experiments at UNILAC verified an enhanced energy loss of heavy ions in a plasma of a factor three at beam energies of 1--6 MeV/u. ... (E = 45 keV/u) it was possible to create a heavy-ion heated plasmas with a high current radio-frequency-quadrupol (RFQ) accelerator. The interaction of this low energy … WebThe energy loss of heavy ions with an energy of 1.4 MeV/u in a hydrogen plasma has been measured. A 20 cm long z -pinch has been used as plasma target. Our data show a strong enhancement of the stopping power of the plasma compared to that of a cold gas …
Beam-plasma interaction experiments with heavy-ion beams
WebDec 20, 2024 · Generally speaking, there are three main mechanisms for the slowing down of heavy particles in fully-ionized plasmas. The first one is the close collision [11 11.J.D. Jackson, Classical Electrodynamics, John Wiley & Sons, Inc, 1975.] between the projectile and the free electron; the second one is the friction-like force caused by plasma … WebSep 1, 1990 · The energy loss of heavy ions in a hydrogen plasma has been measured in an energy range from 1.4 to 6 MeV/u. A z-pinch has been used as a plasma target with a maximum free electron density of 1. ... dr f anwar
[PDF] Energy loss of Fe ions in He plasmas at different …
WebApr 7, 2006 · Gas discharge plasma targets were used for energy loss and charge state measurements of fast heavy ions 5 MeV/u < E{sub kin} < 10 MeV/u in a regime of electron density and temperature up to ... Web@article{osti_5455482, title = {Fast ion stopping power in dense, ionized plasmas. Memorandum report}, author = {Rogerson, J E}, abstractNote = {A model is presented for calculating stopping cross sections for ions in ionized plasma targets. This approach utilizes a local oscillator model to calculate stopping power by bound electrons. Results obtained … WebAug 28, 2006 · The 2p 5 1/2 np' J = 0, 1, 2 and 2p 5 1/2 nf' J = 2 autoionizing Rydberg states (ARS) of Ne have been studied by two-step two-colour photoionization of ground-state neon atoms via the intermediate states 2p 5 3/2 3s J = 1 and 2p 5 1/2 3s' J = 1, followed by time-of-flight ion detection. Strong interference between the direct and virtual intershell … dr fan york hospital