• Chinese Optics Letters
  • Vol. 21, Issue 8, 080002 (2023)
Yimin Zang1, Fanli Wei1, Hee Sung Kim2, and Andy Chong2,*
Author Affiliations
  • 1Department of Electro-Optics and Photonics, University of Dayton, Dayton, Ohio 45469, USA
  • 2Department of Physics, Pusan National University, Busan 46241, Republic of Korea
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    DOI: 10.3788/COL202321.080002 Cite this Article Set citation alerts
    Yimin Zang, Fanli Wei, Hee Sung Kim, Andy Chong, "Temporal manipulation of spatiotemporal optical vortices with an Airy pulse [Invited]," Chin. Opt. Lett. 21, 080002 (2023) Copy Citation Text show less
    Simulation of Airy–STOV wave packet. The TOD of β3z0 = 0.00075 ps3 and the spiral phase of l = 1 have been added to the Gaussian pulse with the full width at half-maximum duration of 45 fs. (a) Normalized intensity profile; (b) phase map.
    Fig. 1. Simulation of Airy–STOV wave packet. The TOD of β3z0 = 0.00075 ps3 and the spiral phase of l = 1 have been added to the Gaussian pulse with the full width at half-maximum duration of 45 fs. (a) Normalized intensity profile; (b) phase map.
    Experimental setup to generate the Airy–STOV.
    Fig. 2. Experimental setup to generate the Airy–STOV.
    Generation of Airy–STOV, β3z0 = 0.00075 ps3, l = 1, Iiso = Imax/15. (a) Simulated iso-intensity plot; (b) experimental iso-intensity plot.
    Fig. 3. Generation of Airy–STOV, β3z0 = 0.00075 ps3, l = 1, Iiso = Imax/15. (a) Simulated iso-intensity plot; (b) experimental iso-intensity plot.
    Comparison between a regular STOV and an Airy–STOV (β3z0 = 0.00075 ps3, l = 1) under a significant GVD of β2z= 0.012 ps2 (3.7LD calculated based on the STOV temporal radius). (a) Simulated regular STOV; (b) simulated Airy–STOV; (c) simulation of the regular STOV under dispersion; (d) simulated dispersion-free propagation of the Airy–STOV; (e) experimental demonstration of dispersion-free propagation of the Airy–STOV.
    Fig. 4. Comparison between a regular STOV and an Airy–STOV (β3z0 = 0.00075 ps3, l = 1) under a significant GVD of β2z= 0.012 ps2 (3.7LD calculated based on the STOV temporal radius). (a) Simulated regular STOV; (b) simulated Airy–STOV; (c) simulation of the regular STOV under dispersion; (d) simulated dispersion-free propagation of the Airy–STOV; (e) experimental demonstration of dispersion-free propagation of the Airy–STOV.
    Simulated and experimental results to demonstrate the self-acceleration effect of the Airy STOV (β3z0 = 0.0005 ps3, l = 1).(a1)–(g1) Simulated intensity plots; (a2)–(g2) simulated phase plots; (a3)–(g3) experimental intensity plots. (a1)–(a3) β2z = 0.009 ps2; (b1)–(b3) β2z = 0.006 ps2; (c1)–(c3) β2z = 0.003 ps2; (d1)–(d3) β2z = 0 ps2; (e1)–(e3) β2z = −0.003 ps2; (f1)–(f3) β2z = −0.006 ps2; (g1)–(g3) β2z = −0.009 ps2.
    Fig. 5. Simulated and experimental results to demonstrate the self-acceleration effect of the Airy STOV (β3z0 = 0.0005 ps3, l = 1).(a1)–(g1) Simulated intensity plots; (a2)–(g2) simulated phase plots; (a3)–(g3) experimental intensity plots. (a1)–(a3) β2z = 0.009 ps2; (b1)–(b3) β2z = 0.006 ps2; (c1)–(c3) β2z = 0.003 ps2; (d1)–(d3) β2z = 0 ps2; (e1)–(e3) β2z = −0.003 ps2; (f1)–(f3) β2z = −0.006 ps2; (g1)–(g3) β2z = −0.009 ps2.
    Simulated (blue solid line) and experimental (red dashed line) phase singularity temporal shift as a function of GVD, β3z0 = 0.0005 ps3.
    Fig. 6. Simulated (blue solid line) and experimental (red dashed line) phase singularity temporal shift as a function of GVD, β3z0 = 0.0005 ps3.
    (a), (c), (e) Simulated and (b), (d), (f) experimental demonstration of the self-healing, Iiso = Imax/5: (a), (b) initial Airy–STOV; (c), (d) disturbed Airy–STOV (center frequency blocked); (e), (f) healed Airy–STOV with GVD of 0.0129 ps2.
    Fig. 7. (a), (c), (e) Simulated and (b), (d), (f) experimental demonstration of the self-healing, Iiso = Imax/5: (a), (b) initial Airy–STOV; (c), (d) disturbed Airy–STOV (center frequency blocked); (e), (f) healed Airy–STOV with GVD of 0.0129 ps2.
    Yimin Zang, Fanli Wei, Hee Sung Kim, Andy Chong, "Temporal manipulation of spatiotemporal optical vortices with an Airy pulse [Invited]," Chin. Opt. Lett. 21, 080002 (2023)
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