2014
DOI: 10.1038/nphoton.2014.79
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Gain dynamics in a soft-X-ray laser amplifier perturbed by a strong injected X-ray field

Abstract: International audienceSeeding soft-X-ray plasma amplifiers with high harmonics has been demonstrated to generate high-brightness soft-X-ray laser pulses with full spatial and temporal coherence. The interaction between the injected coherent field and the swept-gain medium has been modelled. However, no experiment has been conducted to probe the gain dynamics when perturbed by a strong external seed field. Here, we report the first X-ray pump–X-ray probe measurement of the nonlinear response of a plasma amplifi… Show more

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Cited by 28 publications
(13 citation statements)
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“…In this work, we suggest a technique for amplification of a train of attosecond pulses, produced by HHG, in active medium of a plasma-based X-ray laser [33][34][35][36][37][38][39][40][41][42] in the presence of a strong co-propagating IR laser field. An amplification of a single high-order harmonic by the plasma-based X-ray laser has been widely studied before [36][37][38][40][41][42]. But narrow linewidths of X-ray lasers did not allow for joint amplification of several harmonics.…”
mentioning
confidence: 99%
“…In this work, we suggest a technique for amplification of a train of attosecond pulses, produced by HHG, in active medium of a plasma-based X-ray laser [33][34][35][36][37][38][39][40][41][42] in the presence of a strong co-propagating IR laser field. An amplification of a single high-order harmonic by the plasma-based X-ray laser has been widely studied before [36][37][38][40][41][42]. But narrow linewidths of X-ray lasers did not allow for joint amplification of several harmonics.…”
mentioning
confidence: 99%
“…In a direct seeded amplifier scheme, the gain lifetime shall be shorter than the gain recovery lifetime, in order for the stored energy to be transferred only to the seed. In a similar type of seeded plasma x-ray laser experiment [9], the recovery time was measured to be about 2ps. In another experiment reported in [12], using two XRL targets in a master-amplifier configuration, the lifetime of the transient gain in a Ni-like silver medium was determined to be within the range of 3ps.…”
Section: Resultsmentioning
confidence: 99%
“…The enhanced plasma control and the high gain of the 1L2S scheme makes it very attractive for operation as amplifier. Amplification in plasma was first reported in [5] and subsequently addressed in seminal papers such as [6][7][8][9], as they promise higher energy, full coherence, short pulses and polarization control. In order to produce the optimal amplification, the seed spatial extent and the seed pulse duration shall match the ones of the amplifier.…”
Section: Introductionmentioning
confidence: 99%
“…According to the Wiener -Khinchin theorem, this quantity can be obtained from the Fourier transformation of the field correlation function. Using the same normalization as for the intensity (20) and expressing the field correlation function in terms of atomic variables, we find:…”
Section: Field Correlation Function and Spectral Intensitymentioning
confidence: 99%
“…This conclusion was further supported by numerical calculation of the ratio between (C9) and the estimate of (C10). Another way of checking it is to calculate the intensity directly from atomic variables (20) and alternatively from the field correlation function I (a) (τ ) = G (a) (τ, τ ). In the first case, no approximation with regard to (C10) is made and its results agree with the approximate method.…”
mentioning
confidence: 99%