2020
DOI: 10.1038/s41598-020-65477-0
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Narrow-band hard-x-ray lasing with highly charged ions

Abstract: A scheme is put forward to generate fully coherent x-ray lasers based on population inversion in highly charged ions, created by fast inner-shell photoionization using broadband x-ray free-electronlaser (XfeL) pulses in a laser-produced plasma. numerical simulations based on the Maxwell-Bloch theory show that one can obtain high-intensity, femtosecond x-ray pulses of relative bandwidths Δω/ω = 10 −5-10 −7 , by orders of magnitude narrower than in x-ray free-electron-laser pulses for discrete wavelengths down t… Show more

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Cited by 14 publications
(5 citation statements)
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References 95 publications
(163 reference statements)
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“…By knowing these field correlation functions for stochastic FEL pulses, one can predict the properties of C(ω s1 , ω s2 , T ) and retrieve spectroscopic information. Suitable methods have long been utilized to model experiments with stochastic XFEL pulses (143)(144)(145)(146)(147)(148) and simulate chaotic pulses with the correct statistical properties. Figure 7a,b depicts simulated temporal and spectral profiles of stochastic FEL pulses based on the model in References 51, 144, and 145, along with their average intensity profiles.…”
Section: Covariance Signals With Stochastic X-ray Free-electron Lasersmentioning
confidence: 99%
“…By knowing these field correlation functions for stochastic FEL pulses, one can predict the properties of C(ω s1 , ω s2 , T ) and retrieve spectroscopic information. Suitable methods have long been utilized to model experiments with stochastic XFEL pulses (143)(144)(145)(146)(147)(148) and simulate chaotic pulses with the correct statistical properties. Figure 7a,b depicts simulated temporal and spectral profiles of stochastic FEL pulses based on the model in References 51, 144, and 145, along with their average intensity profiles.…”
Section: Covariance Signals With Stochastic X-ray Free-electron Lasersmentioning
confidence: 99%
“…Early optical-laser experiments were also performed with the chaotic pulses available at the time, and simula-tion techniques were developed to model their properties [38]. These methods have long been utilized to model experiments at x-ray FELs [39][40][41][42][43][44]. Pfeifer et al showed that, by using a model starting from random spectral phases, one can simulate chaotic pulses with the correct statistical properties of SASE FEL pulses, including their time and frequency spiky profiles and their energy distribution [40].…”
Section: Modeling Of Stochastic X-ray Free-electron-laser Pulsesmentioning
confidence: 99%
“…( 6) (the term S) can be modeled as a Gaussian white noise following the guidelines of Ref. [16], an approach followed later by others [17,18]. The interest of this approach is that it provides the correct spectral behavior for the field [16].…”
Section: Incident Source -Spontaneous Emissionmentioning
confidence: 99%
“…It is well-known that this problem can be overcome by adding a phenomenological fluctuating polarization source that simulates spontaneous emission. Compared with many calculations of x-ray lasing in gas or plasmas (see for instance Refs [15][16][17][18]) short spatial scales involved in this multilayer context, do not permit the use of the slowly varying envelope approximation so that basic Maxwell equations have to be solved directly. This is done here using the so-called Finite-Difference-Time-Domain (FDTD) method [19].…”
Section: Introductionmentioning
confidence: 99%