By James A. Barnes
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Extra info for A Simulation of the Fluctuations of International Atomic Time
Tissandier LOA, ENSTA, Chemin de la Hunière, Palaiseau cedex, France LPGP, CNRS, LOA, CNRS, ENSTAe, Palaiseau, France F. G. Tomasel Department of Electrical and Computing Engineering, Colorado State University, Fort Collins, CO, USA Advanced Energy Industries, Fort Collis, CO, USA T. Tomita Faculty of Engineering, University of Tokushima, Tokushima, Japan A. Towsend Colorado State University, Fort Collins, CO, USA E. Turgut JILA, University of Colorado, Boulder, CO, USA Faculty of Physics, University of Bucharest, Magurele, Romania R.
A. Pikuz Quantum Beam Science Center, Japan Atomic Energy Agency (JAEA), Kyoto, Japan Joint Institute of High Temperature, Russian Academy of Science, Moscow, Russia A. S. Pirozhkov Quantum Beam Science Center, Japan Atomic Energy Agency (JAEA), Kyoto, Japan M. Pittman LUMAT, CNRS, Universite Paris-Sud, Orsay Cedex, France Campus de lENSTA, Chemin de la Huniere, LASERIX, Universite Paris-Sud, Palaiseau Cedex, France Laboratoire de Physique des Gaz et des Plasmas, Universite Paris-Sud (UMR-CNRS 8578), Cedex, France M.
In recent previous work, we have used a single Advances in High Average Power, 100 Hz Repetition Rate . . 9 nm transition of Ni-like Mo at 100 Hz repetition. 2 mW after calibration of the spectrometer diffraction grating). Here, in order to more efficiently pump the soft x-ray amplifier plasma and allow generation at shorter wavelengths, we made use of a tailored temporal pulse profile that consists of a ∼ 2 ns long, low amplitude ramp that creates and ionizes the plasma and a short duration intense pulse that precedes the main peak of the pulse.