Sensors (Aug 2022)

Nonlinear Propagation and Filamentation on 100 Meter Air Path of Femtosecond Beam Partitioned by Wire Mesh

  • Yuri E. Geints,
  • Olga V. Minina,
  • Ilia Yu. Geints,
  • Leonid V. Seleznev,
  • Dmitrii V. Pushkarev,
  • Daria V. Mokrousova,
  • Georgy E. Rizaev,
  • Daniil E. Shipilo,
  • Irina A. Nikolaeva,
  • Maria V. Kurilova,
  • Nikolay A. Panov,
  • Olga G. Kosareva,
  • Aurélien Houard,
  • Arnaud Couairon,
  • Andrey A. Ionin,
  • Weiwei Liu

DOI
https://doi.org/10.3390/s22176322
Journal volume & issue
Vol. 22, no. 17
p. 6322

Abstract

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High-intensity (∼1 TW/cm2 and higher) region formed in the propagation of ∼60 GW, 90 fs Ti:Sapphire laser pulse on a ∼100 m path in air spans for several tens of meters and includes a plasma filament and a postfilament light channel. The intensity in this extended region is high enough to generate an infrared supercontinuum wing and to initiate laser-induced discharge in the gap between the electrodes. In the experiment and simulations, we delay the high-intensity region along the propagation direction by inserting metal-wire meshes with square cells at the laser system output. We identify the presence of a high-intensity region from the clean-spatial-mode distributions, appearance of the infrared supercontinuum wing, and occurrence of the laser-induced discharge. In the case of free propagation (without any meshes), the onset of the high-intensity zone is at 40–52 m from the laser system output with ∼30 m extension. Insertion of the mesh with 3 mm cells delays the beginning of the high-intensity region to 49–68 m with the same ∼30 m extension. A decrease in the cell size to 1 mm leads to both delay and shrinking of the high-intensity zone to 71–73 m and 6 m, respectively. Three-dimensional simulations in space confirm the mesh-induced delay of the high-intensity zone as the cell size decreases.

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