2010
DOI: 10.3952/lithjphys.50105
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Directly recording diffraction phenomena in the time domain

Abstract: The wave-field produced by a ∼30 fs duration Ti:sapphire oscillator pulse behind a circular aperture and circular opaque disk is measured using the ultrashort-laser-pulse measurement technique, scanning SEA TADPOLE. The high spatial and temporal resolution of the measuring technique enables us to fully image the diffracted field behind the apertures and record the interference pattern produced by the so-called boundary diffraction wave pulses.

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Cited by 3 publications
(2 citation statements)
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“…The U G (P, ω) and U B (P, ω) are given correspondingly by equations ( 5) and (7). u B (P, t) and u G (P, t) are the main and boundary wave pulses [4].…”
Section: The Boundary Wave For a Gaussian Pulsementioning
confidence: 99%
See 1 more Smart Citation
“…The U G (P, ω) and U B (P, ω) are given correspondingly by equations ( 5) and (7). u B (P, t) and u G (P, t) are the main and boundary wave pulses [4].…”
Section: The Boundary Wave For a Gaussian Pulsementioning
confidence: 99%
“…The propagation of an ultrashort pulse exposes it to many such distortions, of which some remain rather surprising. For example, even a simple circular aperture creates a trailing pulse that, in the case of femtosecond laser pulses, is quite distinguishable from the main pulse [4][5][6][7][8][9]. As a result, detailed investigation of ultrashort pulse propagation and focusing is also of fundamental interest in fields that require focusing them, including nonlinear optics, lithography, micro-machinery, biology, and medicine.…”
Section: Introductionmentioning
confidence: 99%