2010
DOI: 10.1364/ol.36.000001
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Precise, real-time, every-single-shot, carrier-envelope phase measurement of ultrashort laser pulses

Abstract: In this Letter we demonstrate a method for real-time determination of the carrier-envelope phase of each and every single ultrashort laser pulse at kilohertz repetition rates. The technique expands upon the recent work of Wittmann and incorporates a stereographic above-threshold laser-induced ionization measurement and electronics optimized to produce a signal corresponding to the carrier-envelope phase within microseconds of the laser interaction, thereby facilitating data-tagging and feedback applications. W… Show more

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Cited by 83 publications
(95 citation statements)
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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%
“…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%
“…Calibration of the peak intensity on target was done with an estimated precision of 10% by separate measurements using single ionization of argon atoms in circularly polarized light [22]. The duration and intensity stability of the pulses were monitored on a shot-to-shot basis by a stereo-above-threshold-ionization phase meter [23,24]. More details on our experimental setup can be found in our previous publications [9,25,26].…”
Section: Methodsmentioning
confidence: 99%
“…Temporal compression of the pulses after the capillary by several bounces from pairs of chirped mirrors and subsequently passing them through a pair of glass wedges for fine-tuning the dispersion results in a pulse duration of ∼ 4.5 fs. The duration and intensity stability of the pulses are monitored on a shot-to-shot basis by a stereo-abovethreshold ionization phase meter [48,49].…”
Section: Methodsmentioning
confidence: 99%