2003
DOI: 10.1088/0034-4885/66/9/203
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Recoil-ion and electron momentum spectroscopy: reaction-microscopes

Abstract: Recoil-ion and electron momentum spectroscopy is a rapidly developing technique that allows one to measure the vector momenta of several ions and electrons resulting from atomic or molecular fragmentation. In a unique combination, large solid angles close to π Microccopes -the "bubble chambers of atomic physics" -mark the decisive step forward to investigate many-particle quantum-dynamics occurring when atomic and molecular systems or even surfaces and solids are exposed to time-dependent external electromagne… Show more

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Cited by 1,751 publications
(1,248 citation statements)
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References 358 publications
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“…The electric field of the laser pulse can be approximated as E(t) = E 0 cos 2 (t/τ) cos(ωt + φ), where E 0 is the field amplitude, ω is the carrier frequency, τ is the pulse duration, and φ is the CEP. Combining a reaction microscope (REMI) 20 with a newly developed phase-tagging technique 21 , we obtained the CEP of the laser pulse for each and every ionization event 22 recorded with the REMI. The laser was focussed to a maximum instantaneous intensity of I 0 = cε 0 E 0 2 = (3.0 ± 0.6)×10 14 W cm − 2 into a cold supersonic gas jet of neutral argon atoms located in the centre of the REMI.…”
Section: Resultsmentioning
confidence: 99%
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“…The electric field of the laser pulse can be approximated as E(t) = E 0 cos 2 (t/τ) cos(ωt + φ), where E 0 is the field amplitude, ω is the carrier frequency, τ is the pulse duration, and φ is the CEP. Combining a reaction microscope (REMI) 20 with a newly developed phase-tagging technique 21 , we obtained the CEP of the laser pulse for each and every ionization event 22 recorded with the REMI. The laser was focussed to a maximum instantaneous intensity of I 0 = cε 0 E 0 2 = (3.0 ± 0.6)×10 14 W cm − 2 into a cold supersonic gas jet of neutral argon atoms located in the centre of the REMI.…”
Section: Resultsmentioning
confidence: 99%
“…A fraction (11 µJ) of the remaining part of the laser beam is focussed with a spherical mirror (f = 25 cm) into a well-localized (1 mm width) and cold supersonic gas jet of neutral argon atoms in the centre of a REMI 20 . Ions and electrons created in the laser focus (~40 µm diameter) are extracted by a weak electric field towards microchannel plate (MCP) detectors equipped with delay line anodes for position readout at the left and right side of the instrument, respectively.…”
Section: Methodsmentioning
confidence: 99%
“…2f) clearly show that the two-electron motion in the reconstructed doubly excited wave packet is highly correlated. Direct experimental observation of such concerted dynamics requires the use of coincidence techniques [25][26][27] and represents a major future goal. At higher intensities (Methods -Intensity Calibration‖; Extended Data Fig.…”
mentioning
confidence: 99%
“…Ref. 25) for direct measurements of the spatial shape of two-(or multi-)electron wave packets as a function of time in the attosecond domain. The extracted state-dependent phases υ n (I) will allow further insight into the coupling among two electrons and how they, collectively or cooperatively, acquire dynamical phases υ n (I) = ∫ΔE n (t)dt, by time-dependent and state(n)-dependent energy-level shifts ΔE n (t) (e.g.…”
mentioning
confidence: 99%
“…The present study serves as an important benchmark for resolving angular momentum quantum states and subsequent decay schemes for theory when both single and multiple electron capture are present. This is a challenge for other experimental measurements, even the well-developed cold target recoil ion momentum spectroscopy [40]. …”
Section: Discussionmentioning
confidence: 99%