Alex B Borisov et al 2007 J. Phys. B: At. Mol. Opt. Phys. 40 F131 doi:10.1088/0953-4075/40/7/F01
Alex B Borisov1, Xiangyang Song1, Ping Zhang1, John C McCorkindale1, Shahab F Khan1, Sankar Poopalasingam1, Ji Zhao1, Yang Dai2 and Charles K Rhodes1,2,3,4
Show affiliationsThe spectral and spatial characteristics of the Xe(L) amplifier at λ ~ 2.9 Å determine an optimum for the scaling of the peak power with channel length. The Xe31+ and Xe32+ (3d → 2p) transition arrays represent two identical spectral optima for amplification, a property stemming from the extremum of spectral components (3245) characteristic of their electron configurations. Adroit matching of the spatial distribution of the intensity characteristic of the propagating 248 nm pulse dynamically generating the self-trapped plasma channel with the intensity required to excite selectively and efficiently the Xe31+ and Xe32+ arrays can also simultaneously maximize the spatial volume of the excitation. The net outcome of this double maximization is an amplifying channel for the optimal transitions that possesses high gain (~100 cm−1), low losses (<10−1cm−1) and a diameter of 15−20 µm, a size sufficient to produce an x-ray pulse energy of ~50−100 mJ from a channel having an average xenon density of ~1020 cm−3 and a length of 1 cm. Since previous studies have experimentally demonstrated the ability to produce a saturated bandwidth of ~60 eV, a magnitude sufficient to support a pulse duration of ~30 as, peak powers Px
1 PW are clearly within the scaling limits of the Xe(L) system. The corresponding peak brightness scaling limit is accordingly bounded from below by Px/λ2
1030 W cm−2 sr−1.
Issue 7 (14 April 2007)
Received 27 December 2006, in final form 8 February 2007
Published 9 March 2007
Alex B Borisov et al 2007 J. Phys. B: At. Mol. Opt. Phys. 40 F131
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