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Get X-ray lasers 2006 : proceedings of the 10th international PDF

By P.V. Nickles, K.A. Janulewicz

ISBN-10: 1402060173

ISBN-13: 9781402060175

ISBN-10: 1402060181

ISBN-13: 9781402060182

The look for table-top and repetitive pump schemes over the last decade has been the driver at the back of the amazing advances established in the course of the tenth foreign convention on X-Ray Lasers, prepared in 2006 in Berlin. The lawsuits of this sequence of meetings represent a complete resource of reference of the stated state-of the-art during this particular region of laser and plasma physics.

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Extra info for X-ray lasers 2006 : proceedings of the 10th international conference, August 20-25, 2006, Berlin, Germany

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2. 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.

In order to find the optimum delay conditions between prepulse and main pulse, a systematic study was conducted to investigate the x-ray laser output intensity as a function of the prepulse-to-main pulse time interval for a range of prepulse amplitudes, as shown in Figure 3 for the case of a Pd target. 5-16 % and main pulse delays of up to 11 ns. 5 J/8 ps, along GRIP path 2 J/15 ps 300-700 ps 300 ps 5 ns 5 ns 800 ps 800 ps Mo 3 J/8 ps 3 J/8 ps 3 J/8 ps Pd Pd Pd X-Ray Lasing Using the GRIP Scheme 41 λ 2nd order Mo Pd Ag Sn Mo Pd Ag Sn (x50) Intensity (counts) 8000 6000 4000 2000 0 5 10 15 20 25 30 Wavelength (nm) Fig.

This repetition is not sufficient for making practical application study. 1 Hz repetition. The zigzag slab is suitable for high repetition operation because the thermal distortion effects in the glass are principally canceled by propagating the zigzag pass. Specification of the power amplifier system is presented in the next 46 Y. Ochi et al. section. The result of x-ray lasing experiment with the Ni-like silver is discussed in section 3. 2 Development of power amplifier using zigzag slab Nd:glass Figure 1 shows a schematic design of the power amplifier system.

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X-ray lasers 2006 : proceedings of the 10th international conference, August 20-25, 2006, Berlin, Germany by P.V. Nickles, K.A. Janulewicz


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