1990
DOI: 10.1016/0168-9002(90)91817-u
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Electron cooling of heavy ions

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Cited by 38 publications
(22 citation statements)
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“…Along their closed orbit with a circumference of 55.4 m, the residual gas pressure is below 1×10 −10 mbar. As in previous experiments [26] at this facility, the ions were merged on each turn in the ring with collinear, velocity-matched or slightly velocity-detuned electron beams of ∼1.5 m length in two straight sections of the TSR: the electron cooler [27][28][29], and the electron target section (ETS) [30].…”
Section: Methodsmentioning
confidence: 99%
“…Along their closed orbit with a circumference of 55.4 m, the residual gas pressure is below 1×10 −10 mbar. As in previous experiments [26] at this facility, the ions were merged on each turn in the ring with collinear, velocity-matched or slightly velocity-detuned electron beams of ∼1.5 m length in two straight sections of the TSR: the electron cooler [27][28][29], and the electron target section (ETS) [30].…”
Section: Methodsmentioning
confidence: 99%
“…The average pressure in the storage ring was 5-10 × 10 −11 mbar during the present measurements. The TSR electron cooler [40,41] was used to apply phase space cooling to the stored He + 2 ion beam [42] and to perform the electron-ion recombination experiments [32,33]. The electron beam is guided by a longitudinal magnetic field (∼0.04 T) and has a diameter of 29.5 mm in the region where the electron and ion beam overlap collinearly, surrounded by a 1.5 m long solenoid magnet.…”
Section: A Ion Beam and Detector Setupmentioning
confidence: 99%
“…When a collinear electron beam [24] is merged with the ion beam (see Fig. 1), electron-ion collisions occur at rest-frame collision energies that can be controlled through the velocity difference between both beams and hence, assuming the ion velocity fixed, through the electron acceleration voltage.…”
Section: Twin Electron Beams In a Magnetic Storage Ringmentioning
confidence: 99%