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Efficient, high-brightness soft-x-ray laser at 21.2 nm
51
Citations
31
References
1997
Year
PhotonicsEngineeringSoft-x-ray LaserPhysicsLasing SystemApplied PhysicsLaser-plasma InteractionLaser Plasma PhysicAtomic PhysicsRelativistic Laser-matter InteractionHigh-brightness Soft-x-ray LaserLasing MediumX-ray Free-electron LaserX-ray OpticX-ray Imaging
In this paper we review the development of a soft-x-ray laser at 21.2 nm, recently carried out at the Laboratoire de Spectroscopie Atomique et Ionique. Amplification is generated by electron collisional pumping on a ${2\mathrm{s}}^{2}$${2\mathrm{p}}^{5}$3p-${2\mathrm{s}}^{2}$${2\mathrm{p}}^{5}$3s, J=0--1 transition in neonlike zinc (${\mathrm{Zn}}^{20+}$). The lasing medium is a \ensuremath{\sim}150 \ensuremath{\mu}m\ifmmode\times\else\texttimes\fi{}2 cm line plasma produced by irradiating slab Zn targets at a net intensity of \ensuremath{\sim}1.4\ifmmode\times\else\texttimes\fi{}${10}^{13}$ W ${\mathrm{cm}}^{\mathrm{\ensuremath{-}}2}$, using a 1.06-\ensuremath{\mu}m, 600-ps-long pulsed laser delivering \ensuremath{\sim}350 J of net energy on the target. Accompanying the driving pulse by a 100-mJ-level prepulse train through deliberately imperfect isolation of the mode-locked laser oscillator, the J=0--1 gain coefficient \ensuremath{\sim}5 ${\mathrm{cm}}^{\mathrm{\ensuremath{-}}1}$ is generated. The emission appears in an \ensuremath{\sim}100-ps burst and precedes the lasing on both the much weaker J=2--1 lines and the x-ray continuum peak. The J=0--1 output source region, the beam spatial profile, and its time history have been measured and their relevance to the kinetics of this lasing system is discussed. A half cavity was implemented and a strong double-pass amplification at 21.2 nm with a 2-cm-long plasma obtained. With the gain-length product achieving \ensuremath{\sim}17.3 according to the particular configuration, saturation was demonstrated, which is confirmed through a schematic model of the level kinetics. To our knowledge, it is the first neonlike soft-x-ray laser where saturation on the J=0--1 line was achieved by using a half-cavity arrangement. Absolute energy measurements indicate \ensuremath{\sim}400 \ensuremath{\mu}J in the half-cavity-generated beam and a peak output power of \ensuremath{\sim}5 MW, which makes this laser one of the most efficient soft-x-ray lasing systems demonstrated to date.
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