2010
DOI: 10.1088/1367-2630/12/4/043020
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Temporal characterization of attosecond pulses emitted from solid-density plasmas

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Cited by 28 publications
(18 citation statements)
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“…In particular, the expected conversion efficiency of a few percent in the low XUV photon energy range creates the possibility to generate mJ-level attosecond trains and isolated attosecond pulses using table-top laser system [44,45]. Temporal characterization of attosecond pulse trains generated on solid targets was recently demonstrated by implementing a second-order autocorrelation [46,47]. The generation and characterization of isolated attosecond pulses using this mechanism would represent a major breakthrough for nonlinear, keV attosecond spectroscopy [39].…”
Section: Hhg For High Xuv Intensitiesmentioning
confidence: 99%
“…In particular, the expected conversion efficiency of a few percent in the low XUV photon energy range creates the possibility to generate mJ-level attosecond trains and isolated attosecond pulses using table-top laser system [44,45]. Temporal characterization of attosecond pulse trains generated on solid targets was recently demonstrated by implementing a second-order autocorrelation [46,47]. The generation and characterization of isolated attosecond pulses using this mechanism would represent a major breakthrough for nonlinear, keV attosecond spectroscopy [39].…”
Section: Hhg For High Xuv Intensitiesmentioning
confidence: 99%
“…For relatively low laser intensities, the so-called coherent wake emission mechanism (CWE) dominates [11,12]. Under these circumstances, it has been recently demonstrated that the harmonic emission leads to temporal bunching with attosecond pulse durations [13,14]. At higher intensities, the relativistic oscillating mirror (ROM) mechanism becomes dominant [15][16][17].…”
Section: Introductionmentioning
confidence: 99%
“…The ROM process can be understood in terms of the relativistic motion of the apparent reflection point, and thus ROM harmonics become dominant when the normalized vector potential a L , which in terms of the focused laser intensity I L is given by a 2 L ¼ I L 2 L =ð1:38 Â 10 18 W cm À2 m 2 Þ, is significantly larger than unity, while for a L & 1 the CWE mechanism is considerably more efficient. While attosecond pulse trains generated using the CWE process have been experimentally observed [17,18], they have been significantly above the transform limited pulse duration. ROM harmonics by contrast possess superior phase characteristics and are therefore better suited to the generation of isolated attosecond pulses with near transform limited pulse durations [19].…”
mentioning
confidence: 99%