4.8 Article

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

期刊

NATURE
卷 524, 期 7566, 页码 446-+

出版社

NATURE PUBLISHING GROUP
DOI: 10.1038/nature14894

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资金

  1. Photon Frontier Network Program
  2. Global COE Program 'Center of Excellence for Atomically Controlled Fabrication Technology' from the Ministry of Education, Sports, Culture, Science and Technology, Japan (MEXT)
  3. [2012B8014]
  4. [2013A8013]
  5. [2013B8020]
  6. [2014A8008]
  7. [25247093]
  8. [23226004]
  9. Grants-in-Aid for Scientific Research [25247093, 23226004] Funding Source: KAKEN

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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(1,2); 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(3,4) have made it possible to generate a hard-X-ray laser (that is, the photon energy is of the order of ten kiloelectronvolts) in anngstrom-wavelength regime(5,6), 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 nanometres7. Here, we use a copper target and report a hard-X-ray inner-shell atomic laser operating at a wavelength of 1.5 angstroms. X-ray free-electron laser pulses with an intensity of about 10(19) watts per square centimetre(7,8) tuned to the copper K-absorption edge produced sufficient population inversion to generate strong amplified spontaneous emission on the copper Ka lines. Furthermore, we operated the X-ray free-electron laser source in a two-colour mode(9), with one colour tuned for pumping and the other for the seed (starting) light for the laser.

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