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Search: WFRF:(Joyeux D)

  • Result 1-7 of 7
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1.
  • Cassou, K., et al. (author)
  • Optimization toward a high-average-brightness soft-x-ray laser pumped at grazing incidence
  • 2007
  • In: Optics Letters. - 0146-9592. ; 32:2, s. 139-141
  • Journal article (peer-reviewed)abstract
    • We report the near-field imaging characterization of a 10 Hz Ni-like 18.9 nm molybdenum soft-x-ray laser pumped in a grazing incidence pumping (GRIP) geometry with a table-top laser driver. We investigate the effect of varying the GRIP angle on the spatial behavior of the soft-x-ray laser source. After multiparameter optimization, we were able to find conditions to generate routinely a high-repetition-rate soft-x-ray laser with an energy level of up to 3 mu J/pulse and to 6 x 10(17) photons/s/mm(2)/mrad(2)/(0.1% bandwidth) average brightness and 1 x 10(28) photons/s/mm(2)/mrad(2)/(0.1% bandwidth) peak brightness. (c) 2006 Optical Society of America.
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2.
  • Kazamias, S, et al. (author)
  • Characterization of a transient collisional Ni-like molybdenum soft x-ray laser pumped in grazing incidence
  • 2008
  • In: Physical Review A (Atomic, Molecular and Optical Physics). - 1050-2947. ; 77:3
  • Journal article (peer-reviewed)abstract
    • We present experimental results from an extensive investigation of a Ni-like Mo X-ray laser pumped in the transient regime and GRIP configuration (GRazing Incidence Pumping). The pump laser is a 10 Hz, 1 J, Ti:Sa laser system. The main diagnostic is a monochromatic near-field imaging system with a 1.7 micron spatial resolution that shows the soft x-ray laser source size and position relative to the target surface. Changes of those characteristics are observed for different GRIP angles, varied between 15◦ and 21◦, while keeping all other parameters constant. Intense lasing is observed routinely at 18.9 nm with up to 3 microjoule output energy and stable operation is demonstrated at 10 Hz. We have investigated the role of several pumping parameters, in particular the relative energy and delay between the long and short pulse. We show that this multi-parameter scan leads to a well-defined optimal regime of operation and better understanding of the GRIP configuration. Finally, as the GRIP scheme requires careful tailoring of the plasma conditions to the specific soft x-ray laser under investigation, we add a prepulse before the plasma producing long pulse to generate large-scale preplasmas. This increases the brightness of the soft x-ray beam and leads to an almost gaussian near-field spatial profile.
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4.
  • Lindau, Filip, et al. (author)
  • Quantitative study of 10 Hz operation of a soft x-ray laser-energy stability and target considerations
  • 2007
  • In: Optics Express. - 1094-4087. ; 15:15, s. 9486-9493
  • Journal article (peer-reviewed)abstract
    • A soft x- ray laser from Ni- like Mo, pumped in grazing incidence ( GRIP), is analyzed with regard to high repetition rate operation. Reliable lasing is obtained, but with significant energy fluctuations attributed mainly to beam pointing jitter from the pump laser. Two modes of operation are compared: continuously moving target and stationary target. With a moving target the soft X- ray output is constant on average, whereas the repeated use of the same target position leads to a pulse energy which increases for several tens of shots. This effect might be caused by improved guiding of the pump laser in the formed groove and the removal, through laser ablation, of the oxide layer on the target surface. (c) 2007 Optical Society of America.
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5.
  • Alessi, D., et al. (author)
  • Spectral Linewidth Measurement of an Injection-Seeded Transient 18.9 nm Soft X-Ray Laser
  • 2011
  • In: 2011 CONFERENCE ON LASERS AND ELECTRO-OPTICS (CLEO). - 9781557529107
  • Conference paper (peer-reviewed)abstract
    • The linewidth of an injection-seeded 18.9nm molybdenum soft x-ray laser (SXRL) was measured to be significantly wider than seeded optical field ionization SXRLs that use gaseous targets, an advantage for the development of sub-picosecond SXRLs.
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6.
  • Meng, L. M., et al. (author)
  • Temporal coherence and spectral linewidth of an injection-seeded transient collisional soft x-ray laser
  • 2011
  • In: Optics Express. - : Optical Society of America. - 1094-4087. ; 19:13, s. 12087-12092
  • Journal article (peer-reviewed)abstract
    • The temporal coherence of an injection-seeded transient 18.9 nm molybdenum soft x-ray laser was measured using a wavefront division interferometer and compared to model simulations. The seeded laser is found to have a coherence time similar to that of the unseeded amplifier, ~1 ps, but a significantly larger degree of temporal coherence. The measured coherence time for the unseeded amplifier is only a small fraction of the pulsewidth, while in the case of the seeded laser it approaches full temporal coherence. The measurements confirm that the bandwidth of the solid target amplifiers is significantly wider than that of soft x-ray lasers that use gaseous targets, an advantage for the development of sub-picosecond soft x-ray lasers.
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7.
  • Merdji, H., et al. (author)
  • Coherence properties of high-order harmonics : Application to high-density laser-plasma diagnostic
  • 2000
  • In: Laser and Particle Beams. - 0263-0346. ; 18:3, s. 495-502
  • Journal article (peer-reviewed)abstract
    • We present two interferometry schemes in the extreme ultraviolet, based on either the wave-front division of a unique harmonic beam (1st scheme) or two spatially separated, phase-locked harmonic sources (2nd scheme). In the first scheme using a Fresnel bimirror interferometer, we measure the degree of spatial coherence of the 13 th harmonic generated in xenon, as a function of different parameters. A high degree of coherence, larger than 0.5, is found for the best conditions in almost the full section of the beam. Then, we demonstrate that the second scheme can be used for interferometry measurements with an ultrahigh time resolution. The 11th harmonic is used to study the spatial variation of the electron density of a laser-produced plasma. Electronic densities higher than 2.10 20 cm -3 are measured.
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  • Result 1-7 of 7

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