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The laser system consists of a Kerr lens mode-locked oscillator, pulse stretcher, multipass amplifier, and pulse compressor. For a review of similar laser systems, see S. Backus, C. G. Durfee, M. M. Murnane, H. C. Kapteyn, Rev. Sci. Instrum. 69, 1207 (1998).
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0343251877
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note
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For x-rays, the relatively small collection angle of the beamline is more than sufficient to accurately image the source (electron beam) without being limited by diffraction.
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18
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0342382365
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note
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-4 of the peak specular intensity.
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19
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0343251876
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note
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The field of the coherent single-cycle infrared pulse will correspond exactly to the solid line in Fig. 4A (minus the constant offset), and the flux will scale as the square of the number of absent electrons in the hole or dark pulse.
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0343687536
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note
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-2 per 0.1% BW at a photon energy of 2 keV.
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21
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0343687534
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note
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This work was supported by the U.S. Department of Energy under contract DE-AC03-76SF00098. The ALS is supported by the Director, Office of Science, Office of Basic Energy Sciences, and Materials Sciences Division of the U.S. Department of Energy under contract DE-AC03-76SF00098 at Lawrence Berkeley National Laboratory. We gratefully acknowledge the use of beamline 6.3.2 and the protein crystallography wiggler (W16) at the ALS and the technical assistance from the ALS Accelerator Physics Group, the ALS Engineering Group, and the ALS operations staff.
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