1996
DOI: 10.1103/physrevlett.76.4328
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Absolute Electron-Impact Ionization Cross Section Measurements Using a Magneto-Optical Trap

Abstract: We present a new method for measuring absolute total electron-impact ionization cross sections. The technique measures fractional loss rates from a magneto-optical trap due to electron-impact ionization. The method requires only relative measurements of the number of target atoms and therefore eliminates a major source of difficulty in previous experiments. We report total ionization cross sections of Rb for electron energies from 50 to 500 eV. [S0031-9007(96)00306-7]

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Cited by 56 publications
(36 citation statements)
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“…These measurements involve collisions of trapped neutral particles with neutral atoms and molecules [20][21][22][23][24], electron beams [25][26][27], and trapped ions [28][29][30]. Photoionization cross sections have also been investigated though measurements of trap loss rates [31][32][33].…”
mentioning
confidence: 99%
“…These measurements involve collisions of trapped neutral particles with neutral atoms and molecules [20][21][22][23][24], electron beams [25][26][27], and trapped ions [28][29][30]. Photoionization cross sections have also been investigated though measurements of trap loss rates [31][32][33].…”
mentioning
confidence: 99%
“…(In photoionization the 3 =1 ratio is 15 times larger at 424 eV, easing the signal/background requirements.) The use of ultracold atom targets for electron scattering studies was pioneered for absolute ionization cross section measurements [28]. The basic strategy was to prepare a target of ultracold lithium atoms at the center of a time-of-flight (TOF) ion spectrometer.…”
mentioning
confidence: 99%
“…The atoms are located far from the discharge source at the center of a 3D magneto-optical trap (MOT) which is loaded from a bright beam of He2 3 S atoms, also produced by laser-cooling techniques. Atom trap-based techniques have been used previously for electron collision studies, but not with metastable excited atomic species such as He2 3 S. Previous experiments have involved total cross section measurements on Rb [12] and Cs [13] and total ionization measurements on Rb [14]. A similar experimental approach has been used here, although the light mass and strong Penning ionization of the He atoms provides for substantially greater difficulties in maintaining significant metastable atom densities.…”
mentioning
confidence: 99%