4.8 Article

Controlling the polarization and vortex charge of attosecond high-harmonic beams via simultaneous spin-orbit momentum conservation

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NATURE PHOTONICS
卷 13, 期 2, 页码 123-+

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NATURE PUBLISHING GROUP
DOI: 10.1038/s41566-018-0304-3

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资金

  1. Department of Energy BES Award [DE-FG02-99ER14982]
  2. MURI grant from the Air Force Office of Scientific Research [FA9550-16-1-0121]
  3. National Science Foundation Graduate Research Fellowships [DGE-1144083]
  4. Junta de Castilla y Leon [SA046U16]
  5. Ministerio de Economia y Competitividad [FIS2013-44174-P, FIS2016-75652-P]
  6. 2017 Leonardo Grant for Researchers and Cultural Creators, BBVA Foundation
  7. Ministerio de Educacion, Cultura y Deporte [FPU16/02591]
  8. Marie Sklodowska-Curie Grant [702565]
  9. European Regional Development Fund (ERDF)
  10. Barcelona Supercomputing Center [RES-AECT-2014-2-0085]
  11. Marie Curie Actions (MSCA) [702565] Funding Source: Marie Curie Actions (MSCA)
  12. U.S. Department of Energy (DOE) [DE-FG02-99ER14982] Funding Source: U.S. Department of Energy (DOE)

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Optical interactions are governed by both spin and angular momentum conservation laws, which serve as a tool for controlling light-matter interactions or elucidating electron dynamics and structure of complex systems. Here, we uncover a form of simultaneous spin and orbital angular momentum conservation and show, theoretically and experimentally, that this phenomenon allows for unprecedented control over the divergence and polarization of extreme-ultraviolet vortex beams. High harmonics with spin and orbital angular momenta are produced, opening a novel regime of angular momentum conservation that allows for manipulation of the polarization of attosecond pulses-from linear to circular-and for the generation of circularly polarized vortices with tailored orbital angular momentum, including harmonic vortices with the same topological charge as the driving laser beam. Our work paves the way to ultrafast studies of chiral systems using high-harmonic beams with designer spin and orbital angular momentum.

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