2007
DOI: 10.1063/1.2771518
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Cold electron and ion beams generated from trapped atoms

Abstract: A novel way of creating low-temperature electron and ion beams is demonstrated. The beams are generated by converting a laser-cooled atom cloud to a highly excited Rydberg gas, which subsequently develops into an ultracold plasma. Charged particles are extracted from the Rydberg gas and the plasma by a pulsed electric field. The properties of the resulting electron and ion pulses are experimentally studied. Pulses of a few hundred ns duration containing a few pC of charge were observed. Upper limits for the te… Show more

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Cited by 48 publications
(28 citation statements)
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“…Cold atom sources have generated electron bunches with high coherence, up to 10 nm at the source 11 . The bunch charge can be a few picocoulombs, sufficient for single-shot imaging of nanocrystals of biomolecules 12,13 , but the nanosecond duration of the electron bunches has been too long for observation of useful dynamics.…”
mentioning
confidence: 99%
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“…Cold atom sources have generated electron bunches with high coherence, up to 10 nm at the source 11 . The bunch charge can be a few picocoulombs, sufficient for single-shot imaging of nanocrystals of biomolecules 12,13 , but the nanosecond duration of the electron bunches has been too long for observation of useful dynamics.…”
mentioning
confidence: 99%
“…With a cold atom source, electrons are typically produced by photionization of cold atoms in a two-step process, with microsecond laser excitation to an intermediate atomic state and nanosecond ionization of the excited atoms 11,13 . Timedependent extraction fields can be used to reduce the electron bunch length 14 , but picosecond switching times are not feasible.…”
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confidence: 99%
“…After first preliminary experiments [8], the UCIS potential of delivering beams of LMIS brightness was recently demonstrated [9]. In this Letter we present detailed TOF energy spread measurements on rubidium ion bunches extracted from a UCIS.…”
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confidence: 99%
“…This implies that the minimal transverse normalized emittance that can be achieved scales with the square root of bunch charge: ϵ ∝ ⊥ N . An interesting new development is the ultracold electron source, which is based on near-threshold photoionization of laser-cooled atomic gases [7][8][9][10][11][12][13][14][15]. The ultracold source is characterized by effective temperatures as low as ∼ T 10 K. This implies that for the same source size, and thus the same bunch charge, bunches can be produced with an emittance 1-2 orders of magnitude lower than by photoemission.…”
Section: Introductionmentioning
confidence: 99%