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      Atomic inner-shell laser at 1.5-ångström wavelength pumped by an X-ray free-electron laser.

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          Abstract

          Since the invention of the first lasers in the visible-light region, research has aimed to produce short-wavelength lasers that generate coherent X-rays; the shorter the wavelength, the better the imaging resolution of the laser and the shorter the pulse duration, leading to better temporal resolution in probe measurements. Recently, free-electron lasers based on self-amplified spontaneous emission have made it possible to generate a hard-X-ray laser (that is, the photon energy is of the order of ten kiloelectronvolts) in an ångström-wavelength regime, enabling advances in fields from ultrafast X-ray spectrosopy to X-ray quantum optics. An atomic laser based on neon atoms and pumped by a soft-X-ray (that is, a photon energy of less than one kiloelectronvolt) free-electron laser has been achieved at a wavelength of 14 nanometres. Here, we use a copper target and report a hard-X-ray inner-shell atomic laser operating at a wavelength of 1.5 ångströms. X-ray free-electron laser pulses with an intensity of about 10(19) watts per square centimetre tuned to the copper K-absorption edge produced sufficient population inversion to generate strong amplified spontaneous emission on the copper Kα lines. Furthermore, we operated the X-ray free-electron laser source in a two-colour mode, with one colour tuned for pumping and the other for the seed (starting) light for the laser.

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          Most cited references24

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          Collective instabilities and high-gain regime in a free electron laser

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            Demonstration of a Soft X-Ray Amplifier

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              Femtosecond electronic response of atoms to ultra-intense X-rays.

              An era of exploring the interactions of high-intensity, hard X-rays with matter has begun with the start-up of a hard-X-ray free-electron laser, the Linac Coherent Light Source (LCLS). Understanding how electrons in matter respond to ultra-intense X-ray radiation is essential for all applications. Here we reveal the nature of the electronic response in a free atom to unprecedented high-intensity, short-wavelength, high-fluence radiation (respectively 10(18) W cm(-2), 1.5-0.6 nm, approximately 10(5) X-ray photons per A(2)). At this fluence, the neon target inevitably changes during the course of a single femtosecond-duration X-ray pulse-by sequentially ejecting electrons-to produce fully-stripped neon through absorption of six photons. Rapid photoejection of inner-shell electrons produces 'hollow' atoms and an intensity-induced X-ray transparency. Such transparency, due to the presence of inner-shell vacancies, can be induced in all atomic, molecular and condensed matter systems at high intensity. Quantitative comparison with theory allows us to extract LCLS fluence and pulse duration. Our successful modelling of X-ray/atom interactions using a straightforward rate equation approach augurs favourably for extension to complex systems.
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                Author and article information

                Journal
                Nature
                Nature
                1476-4687
                0028-0836
                Aug 27 2015
                : 524
                : 7566
                Affiliations
                [1 ] Institute for Laser Science, University of Electro-Communications, Chofu, Tokyo 182-8585, Japan.
                [2 ] RIKEN SPring-8 Center, Sayo, Hyogo 679-5148, Japan.
                [3 ] Japan Synchrotron Radiation Research Institute (JASRI), Sayo, Hyogo 679-5198, Japan.
                [4 ] Graduate School of Engineering, Osaka University, Suita, Osaka 565-0871 Japan.
                [5 ] Department of Precision Engineering, The University of Tokyo, Bunkyo, Tokyo 113-8656, Japan.
                [6 ] Department of Physics, Kyoto University, Sakyo-ku, Kyoto 606-8502, Japan.
                Article
                nature14894
                10.1038/nature14894
                26310765
                344f59db-5e3b-43e3-ba43-754b57f6f8a1
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