2001
DOI: 10.1016/s0022-4073(00)00108-4
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Further simulations of the gain in a K XIX/Cl XVII resonantly photopumped X-ray Laser

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Cited by 4 publications
(3 citation statements)
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“…3, any deviations from the ideal conditions, i.e., those at which enhancement peaks, will result in a reduction in enhancement. This reflects the requirement for a high population of He-like K and H-like Cl, a necessity for the pumping line to be optically thick, maximizing absorption, and yet low enough density that photopumping is not destroyed by collisional deexcitation [19]. This experiment, relying on long pulse heating of a finite size laser target, will be subject to spatial and temporal gradients in temperature and density.…”
Section: Fig 3 Contour Plot Showing Cretin Calculated Increases In mentioning
confidence: 99%
“…3, any deviations from the ideal conditions, i.e., those at which enhancement peaks, will result in a reduction in enhancement. This reflects the requirement for a high population of He-like K and H-like Cl, a necessity for the pumping line to be optically thick, maximizing absorption, and yet low enough density that photopumping is not destroyed by collisional deexcitation [19]. This experiment, relying on long pulse heating of a finite size laser target, will be subject to spatial and temporal gradients in temperature and density.…”
Section: Fig 3 Contour Plot Showing Cretin Calculated Increases In mentioning
confidence: 99%
“…R r a/b is the radiative rate from a to b. In addition to the rate equations X a Z a ðtÞn a ðtÞ ¼ n e (2) gives the total electron number density where Z a is the degree of ionisation (the number of ionised electrons arising from the ion in level a) where n e is the electron number density. In some cases where there is reason to believe that the populations have reached a steady-state then the problem can be simplified by solving equations (1) and (2) together with E-mail address: s.rose@imperial.ac.uk…”
Section: Population Kinetics Including a Radiation Fieldmentioning
confidence: 99%
“…However there has been much theoretical work on both the degree to which the two lines coincide (for example [1,27] and on the calculation of the operation of the scheme [20,21] and references contained therein). Possible reasons for this lack of experimental success include the differential Doppler shift between the pumping and pumped plasma and an overestimate of the brightness in the pumping line (possibly due to velocity gradients in the pumping plasma producing much larger effective line widths than have been assumed [2,3,6,[23][24][25]37,38]). Whilst not resulting in gain, other experiments have demonstrated direct photopumping of one plasma by another.…”
Section: Narrow-band Photopumpingmentioning
confidence: 99%