Download X-ray lasers 2006 : proceedings of the 10th international by P.V. Nickles, K.A. Janulewicz PDF
By P.V. Nickles, K.A. Janulewicz
The look for table-top and repetitive pump schemes over the past decade has been the driver in the back of the remarkable advances tested throughout the tenth overseas convention on X-Ray Lasers, prepared in 2006 in Berlin. The lawsuits of this sequence of meetings represent a accomplished resource of reference of the stated state-of the-art during this particular region of laser and plasma physics.
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Additional info for X-ray lasers 2006 : proceedings of the 10th international conference, August 20-25, 2006, Berlin, Germany
Sample text
3. 4. 5. V. N. Shlyaptsev: 'Formation of a population inversion of transitions in Ne-like ions in steady-state and transient plasmas', Sov. J. Quant. Electron. 19, 1606, 1989. P. : 'Saturated operation of a transient collisional x-ray laser', Phys. Rev. A 57, 4778, 1998; J. : 'Gain saturation regime for laser-driven tabletop, transient Ni-like ion X-ray lasers', Phys. Rev. Lett. 84, 4834, 2000. N. : “Numerical study of transient and capillary x-ray lasers and their applications”, Proc. SPIE, Vol.
7 nm laser intensity from a Pd target vs. main pulse delay, for a range of prepulse amplitudes. This page intentionally blank 42 J. Balmer et al. This is in distinct difference to the results of Refs. 3 and 4, where substantially narrower temporal windows of ~50 ps and ~800 ps have been reported for lasing in Mo and Ag, respectively. Of course, those experiments were driven either just above the threshold for lasing (Mo) or just above saturation (Ag), with main pulse energies of ~100 mJ and ~1 J, respectively.
The smaller incidence angle of the second pulse is used, the more uniform electron density in the plasma is generated. 0×1020 cm−3, which is the required electron density for the Ne-like Ti x-ray laser, gives the widest gain region about 70 µm. The longer time the plasma expands before the second pulse, the wider the flat stage of electron density distribution is, as shown in Fig. 2 (b). But if the interval is too long, for example 7 ns, the electron density at the flat stage will be further reduced.