| 1. |
- Miranda, Miguel, et al.
(författare)
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All-optical measurement of the complete waveform of octave-spanning ultrashort light pulses
- 2019
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Ingår i: Optics Letters. - 0146-9592. ; 44:2, s. 191-194
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Tidskriftsartikel (refereegranskat)abstract
- We demonstrate the complete temporal characterization of the optical waveform of visible near-infrared octave-spanning ultrashort laser pulses, using an all-optical, all-solid-state, and fully inline dispersion-scan device based only on second-harmonic generation.
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| 2. |
- Hernandez-Garcia, C., et al.
(författare)
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Carrier-envelope-phase insensitivity in high-order harmonic generation driven by few-cycle laser pulses
- 2015
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Ingår i: Optics Express. - 1094-4087. ; 23:16, s. 21497-21508
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Tidskriftsartikel (refereegranskat)abstract
- We present evidence for self-stabilization of the relative spectral phase of high-order harmonic emission against intensity variations of the driving field. Our results demonstrate that, near the laser focus, phase matching of the harmonic field from a macroscopic target can compensate for the intensity dependence of the intrinsic phase of the harmonics emitted by a single radiator. As a consequence, we show experimentally and theoretically the insensitivity of the harmonic spectra produced at the laser focus against variations of the carrier-envelope phase (CEP) of a sub-two-cycle driving field. In addition, the associated attosecond pulse trains exhibit phase locking against CEP changes of the few-cycle driver. (C) 2015 Optical Society of America
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| 3. |
- Holgado, W., et al.
(författare)
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Continuous spectra in high-harmonic generation driven by multicycle laser pulses
- 2016
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Ingår i: Physical Review A (Atomic, Molecular and Optical Physics). - 1050-2947. ; 93:1
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Tidskriftsartikel (refereegranskat)abstract
- We present observations of the emission of XUV continua in the 20-37-eV region by high-harmonic generation with 4-7-fs pulses focused onto a Kr gas jet. The underlying mechanism relies on coherent control of the relative delays and phases between individually generated attosecond pulses, achievable by adjusting the chirp of the driving pulses and the interaction geometry. Under adequate negative chirp and phase-matching conditions, the resulting interpulse interference yields a continuum XUV spectrum, which is due to both microscopic and macroscopic (propagation) contributions. This technique opens the route for modifying the phase of individual attosecond pulses and for the coherent synthesis of XUV continua from multicycle driving laser pulses without the need of an isolated attosecond burst.
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| 4. |
- Silva, Francisco, et al.
(författare)
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Monolithic single-shot dispersion-scan : A new tool for real-time measurement and optimization of femtosecond pulses
- 2017
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Ingår i: The European Conference on Lasers and Electro-Optics, CLEO_Europe 2017. - 9781509067367
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Konferensbidrag (refereegranskat)abstract
- The precise characterization of femtosecond laser pulses is as challenging as their generation and a topic of intense research. Dispersion-scan (d-scan) [1] is a recently established technique where the spectrum of a nonlinear signal, e.g., second-harmonic generation (SHG), is measured as a function of dispersion applied to the pulse. The spectral phase of the pulse can then be retrieved from the resulting 2D trace using an iterative algorithm. An important implementation of d-scan, based on a chirped mirror and wedge compressor, involves progressively moving one of the wedges around the maximum compression point and acquiring the resulting SHG spectrum for each insertion with a standard spectrometer. This robust and fully inline approach, which does not require any beamsplitting or temporal delays, has enabled the simultaneous compression and measurement of pulses down to single-cycle durations [2-4], but its scanning nature precludes single-shot operation. A single-shot d-scan variant that explores the spatially dependent dispersion of a glass prism was successfully demonstrated with 3.2 fs pulses [5], but the relatively small amount of dispersion that can be introduced by a single prism limits its use to few-cycle pulses.
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