1995
DOI: 10.1109/2944.473682
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Discharge-driven 46.9-nm amplifier with gain-length approaching saturation

Abstract: Abstract-Gain length products up to gl w 14 for the J = 0-1 line of Ne-like Ar at 46.9 nm have been achieved in 15-cmlong plasma columns generated by a fast capillary discharge. Amplification in plasma columns up to 20 cm in length was investigated. The laser line intensity is observed to increase exponentially for plasma lengths of up to 15 cm, above which it is observed to saturate. The saturation behavior is discussed.

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Cited by 18 publications
(9 citation statements)
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“…A fit of the data corresponding to plasma column lengths up to 11.5 cm with the Linford formula [18] yields a gain coefficient g 1.16 cm 21 , a gain value that is close to that of previous measurements [15]. Saturation of the intensity is observed at a gainlength product of about 14.…”
mentioning
confidence: 51%
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“…A fit of the data corresponding to plasma column lengths up to 11.5 cm with the Linford formula [18] yields a gain coefficient g 1.16 cm 21 , a gain value that is close to that of previous measurements [15]. Saturation of the intensity is observed at a gainlength product of about 14.…”
mentioning
confidence: 51%
“…Recent optimization of the capillary discharge scheme, which has the advantages of a relatively large gain volume and long gain duration, allowed amplification at 46.9 nm to reach 14 gain-length products [15], but no demonstration of substantial laser energy extraction was realized. In this Letter we report the generation of laser pulse energies up to 30 mJ at 46.9 nm in the plasma column of a fast compressional capillary discharge and the first clear evidence of gain saturation of a table-top soft x-ray amplifier.…”
mentioning
confidence: 99%
“…1, corresponding to the amplification of the 46.9 nm line of Ne-like Ar in a discharge-created plasma, the laser line intensity increases with a gain coefficient g Ϸ0.92 cm Ϫ1 until saturation is reached at lϷ15 cm. 70,83 In conclusion, to achieve saturated soft x-ray amplification in a single-or double-pass amplifier the gain coefficient must be, depending on the length of the plasma, 1-3 orders of magnitude larger than that typically encountered in most visible gas lasers. 88 Moreover, the fundamental physics of the generation of amplification by stimulated emission determines a dramatic upward scaling of the power density deposition required to obtain substantial gain at ultrashort wavelengths.…”
Section: A Pump Power Requirements and Scaling Lawsmentioning
confidence: 99%
“…While research towards the development of table-top x-ray lasers based on nanosecond pulse laser drivers continues to date, 80 much of the recent effort has shifted towards the use of small-scale high power ultrafast laser drivers [74][75][76][77][78]216 and compact high power discharges. 17,[68][69][70][81][82][83]124,[152][153][154][155] New opportunities for the efficient pumping of table-top soft x-ray lasers have arisen from the development of compact, very high power ultrafast optical lasers based on the technique of chirped-pulse amplification ͑CPA͒, and from the demonstration of highly ionized capillary discharge plasma columns of unprecedented axial uniformity. CPA of ultrashort laser pulses presently allows for the generation of multiterawatt peak powers from tabletop systems operating at repetition rates of typically 10 Hz.…”
Section: Present Status Of Table-top Driversmentioning
confidence: 99%
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