1989
DOI: 10.1070/qe1989v019n12abeh009835
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Formation of a population inversion of transitions in Ne-like ions in steady-state and transient plasmas

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Cited by 88 publications
(28 citation statements)
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“…A recently demonstrated variation of the collisional electron excitation scheme takes advantage of the much larger population inversions that can be obtained under rapid transient excitation. [76][77][78] It was first recognized by Afanasiev and Shlyaptsev 146 that gain coefficients that are 1-2 orders of magnitude larger than those obtained for the same transition in the quasisteady state regime can be produced for a short period of time ͑typically subpicosecond to tens of picoseconds͒ by heating the plasma at a rate faster than the relaxation rate of the excited states. The larger gain coefficients are a consequence of several phenomena that, for a short period following rapid transient heating, contribute to generate a much higher population inversion.…”
Section: Transient Electron Collisional Excitationmentioning
confidence: 99%
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“…A recently demonstrated variation of the collisional electron excitation scheme takes advantage of the much larger population inversions that can be obtained under rapid transient excitation. [76][77][78] It was first recognized by Afanasiev and Shlyaptsev 146 that gain coefficients that are 1-2 orders of magnitude larger than those obtained for the same transition in the quasisteady state regime can be produced for a short period of time ͑typically subpicosecond to tens of picoseconds͒ by heating the plasma at a rate faster than the relaxation rate of the excited states. The larger gain coefficients are a consequence of several phenomena that, for a short period following rapid transient heating, contribute to generate a much higher population inversion.…”
Section: Transient Electron Collisional Excitationmentioning
confidence: 99%
“…Transient gains in excess of 100 cm Ϫ1 have been predicted theoretically. [146][147][148][149][150] The shortlived transient population inversions, which are pumped directly from the ground state by electron collisional excitation, last until collisions redistribute the populations among levels. Following this short transient period of high population inversion the gain decreases until the laser level populations finally reach the quasisteady state value.…”
Section: Transient Electron Collisional Excitationmentioning
confidence: 99%
“…The latter is of concern in the longitudinal pumping geometry where all of the laser energy required for the full plasma column has to be propagated through the initial parts of the plasma. The RADEX simulation code [17] predicts that the absorption in the gain region can be increased from 5 -8% for transverse pumping to as high as 50 -70% for the GRIP geometry [9,10]. To illustrate the increased absorption, Fig.…”
Section: Grazing Incidence Pumping Geometrymentioning
confidence: 99%
“…2 The transient collisional excitation scheme as described by Afanasiev and Shlyaptsev has been proposed to achieve tabletop operation for laser-driven schemes. 3 This utilizes two laser pulses where a long nanosecond pulse at 10 12 W cm -2 generates the plasma and creates the required closed shell Ne-like or Ni-like ionization conditions. After a delay to allow for plasma cooling and expansion which is desirable for both optimum pumping and ray propagation along the plasma column, a second much shorter 1 ps laser pulse at 10 15 W cm -2 rapidly generates a transient population inversion.…”
Section: Introductionmentioning
confidence: 99%