2008
DOI: 10.1007/s00340-008-2987-5
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Interferometric long-term stabilization of a delay line: a tool for pump–probe photoelectron–photoion-coincidence spectroscopy on the attosecond time scale

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Cited by 17 publications
(10 citation statements)
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“…Other schemes are possible using, for instance, up to three photodiodes to track the interferometer displacement. 58 In our case, the green laser beam enters the interferometer from the back side of the first BS (see top left BS and green lines in Fig. 2).…”
Section: B Active Stabilizationmentioning
confidence: 97%
“…Other schemes are possible using, for instance, up to three photodiodes to track the interferometer displacement. 58 In our case, the green laser beam enters the interferometer from the back side of the first BS (see top left BS and green lines in Fig. 2).…”
Section: B Active Stabilizationmentioning
confidence: 97%
“…This requirement, combined with the long-acquisition times typical of coincidence measurements, represents a technical challenge for the implementation and development of attosecond coincidence spectroscopy. In many pump-probe measurements, a non-copropagating geometry, which requires an active stabilization setup [12][13][14][15][16][17], is used. This solution, however, adds complexity to the experimental apparatus.…”
Section: Introductionmentioning
confidence: 99%
“…The advantage of this design is pumpprobe stability, because the delay between the XUV beam and near-infrared (NIR) beam is produced by only one optic: a combined XUV multilayer coated mirror and Ag coated mirror [8,[12][13][14]. Furthermore, the delay can be stabilized with an active feedback loop (stability of 46 as over 33 hours) in order to counteract any slow drifts [15]. In addition, the multilayer mirror can be designed to select specific attosecond frequencies.…”
Section: Collinear Setupmentioning
confidence: 99%