4.8 Article

Conservation of Torus-knot Angular Momentum in High-order Harmonic Generation

Journal

PHYSICAL REVIEW LETTERS
Volume 122, Issue 20, Pages -

Publisher

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevLett.122.203201

Keywords

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Funding

  1. Cellex-ICFO-MPQ fellowship
  2. Spanish Ministry MINECO [FIS2016-79508-P, SEV-2015-0522]
  3. European Social Fund
  4. Fundacio Cellex
  5. Generalitat de Catalunya (AGAUR Grant) [2017 SGR 1341]
  6. Generalitat de Catalunya (CERCA/Program)
  7. ERC AdG OSYRIS
  8. EU FETPRO QUIC
  9. National Science Centre, Poland-Symfonia Grant [2016/20/W/ST4/00314]
  10. Comunidad de Madrid through TALENTO Grant [2017-T1/IND-5432]
  11. Junta de Castilla y Leon [SA046U16]
  12. Ministerio de Economia y Competitividad [FIS2013-44174-P, FIS2016-75652-P]
  13. 2017 Leonardo Grant for Researchers and Cultural Creators
  14. BBVA Foundation
  15. Ministerio de Ciencia, Innovacion y Universidades [RYC-2017-22745]
  16. Ministerio de Educacion, Cultura y Deporte [FPU16/02591]
  17. Department of Energy BES Award [DE-FG02-99ER14982]
  18. DARPATEE Award [D18AC00017]
  19. Barcelona Supercomputing Center [RES-AECT-2014-2-0085]
  20. European Regional Development Fund (ERDF)

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High-order harmonic generation stands as a unique nonlinear optical up-conversion process, mediated by a laser-driven electron recollision mechanism, which has been shown to conserve energy, linear momentum, and spin and orbital angular momentum. Here, we present theoretical simulations that demonstrate that this process also conserves a mixture of the latter, the torus-knot angular momentum J(gamma), by producing high-order harmonics with driving pulses that are invariant under coordinated rotations. We demonstrate that the charge J(gamma) of the emitted harmonics scales linearly with the harmonic order, and that this conservation law is imprinted onto the polarization distribution of the emitted spiral of attosecond pulses. We also demonstrate how the nonperturbative physics of high-order harmonic generation affect the torus-knot angular momentum of the harmonics, and we show that this configuration harnesses the spin selection rules to channel the full yield of each harmonic into a single mode of controllable orbital angular momentum.

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