2006
DOI: 10.1016/j.nima.2006.09.055
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A laser ablation ion source for gas cell studies

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Cited by 4 publications
(2 citation statements)
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“…The reason for the difference in the chemical evolution of the primary ionization in the NSCL and the SHIPTRAP gas cells is now apparent. The shortest drift time from the midpoint of the NSCL gas cell at 1 bar of t $ 50 ms (l $ 20 cm 2 /s/V and E $ 25 V/ cm, see for example [27]), is longer than the mean lifetime for charge exchange at this pressure. On the other hand, the drift time reported for the SHIPTRAP gas cell of t 6 10 ms [21] is fifty times shorter than the estimated mean lifetime for reactions in this system (s $ 500 ms) at the same ppb level of contamination.…”
Section: Ion Chemistrymentioning
confidence: 97%
“…The reason for the difference in the chemical evolution of the primary ionization in the NSCL and the SHIPTRAP gas cells is now apparent. The shortest drift time from the midpoint of the NSCL gas cell at 1 bar of t $ 50 ms (l $ 20 cm 2 /s/V and E $ 25 V/ cm, see for example [27]), is longer than the mean lifetime for charge exchange at this pressure. On the other hand, the drift time reported for the SHIPTRAP gas cell of t 6 10 ms [21] is fifty times shorter than the estimated mean lifetime for reactions in this system (s $ 500 ms) at the same ppb level of contamination.…”
Section: Ion Chemistrymentioning
confidence: 97%
“…The laser ablation ion source can produce most of the stable/radioactive metallic ions by local heating of a metal target with a laser in order to sputter ions from the surface into the gas [115,116]. Figure 3.7 shows a schematic view of the laser ablation ion-production principle.…”
Section: Internal Ion Sourcesmentioning
confidence: 99%