2017
DOI: 10.1139/cjp-2016-0716
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Time-dependent potential functions to stretch the time distributions of ion pulses ejected from EBIST

Abstract: Electron beam ion sources and traps (EBIST) produce and trap highly charged atomic ions with an electron beam of high current density. The ions are confined in the radial space-charge potential of the electron beam and a long square-shaped axial electrostatic potential well. An important field of application of EBIST is charge breeding of highly charged ions at radioactive ion beam facilities. There, highly charged radioactive isotopes are accelerated by particle accelerators for experiments in nuclear astroph… Show more

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Cited by 10 publications
(6 citation statements)
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“…With the axial potential set to 1.6 kV, the ion-cloud radius becomes the same as the electron-beam radius at the compensation ratio of 0.69. A Maxwell-Boltzmann distribution with 3-degree-of-freedom [10] was used for generating the initial ion energy distribution presented in Figure 2. A most probable ion kinetic energy per charge was set to be 10% of each axial potential, as 1.5Ti/q ≈ 0.1eVwell.…”
Section: Electron-and Ion-beam Simulationsmentioning
confidence: 99%
“…With the axial potential set to 1.6 kV, the ion-cloud radius becomes the same as the electron-beam radius at the compensation ratio of 0.69. A Maxwell-Boltzmann distribution with 3-degree-of-freedom [10] was used for generating the initial ion energy distribution presented in Figure 2. A most probable ion kinetic energy per charge was set to be 10% of each axial potential, as 1.5Ti/q ≈ 0.1eVwell.…”
Section: Electron-and Ion-beam Simulationsmentioning
confidence: 99%
“…The energy distribution of 85 Rb 9+ ions inside the trap was measured with a method derived from [4]. The idea is to split the ion bunch into two components by using a three-level extraction function: trap closed (V = V high ), partially open (V = V p ) over a time t p , and open (V = V low ).…”
Section: Energy Distribution Measurementsmentioning
confidence: 99%
“…Stretching the pulses can be accomplished by lowering the ejection barrier potential over a long time period with a time-dependent voltage function resembling a ramp. Theoretical studies were conducted in [35] and test results using this stretching scheme were presented in [21,30]. Highly charged ions produced from injected and residual gas, 84 Kr 26þ and 40 Ar 16þ , respectively, were used for these tests by detecting ions with an MCP located after the Q=A separator.…”
Section: Stretching Of Ejected Ion Pulsesmentioning
confidence: 99%
“…Ar 17þ and 46 K 18þ ejected with a linear function over 120 ms were observed to exit the trap within a narrow distribution of approximately 10-20 ms half-way or over the last portion of the ramp. To maximize the ion spread (and make efficient use of the time available for ejection), the barrier potential has to be first lowered rapidly at the beginning of the ejection time to reach the maximum of the energy distribution in the trapping potential [35]. Then, the lowering rate must be reduced for a slow release of ions as needed.…”
mentioning
confidence: 99%