• Photonics Research
  • Vol. 9, Issue 8, 1513 (2021)
Wanvisa Talataisong1、2、*, Jon Gorecki1、3, Lieke D. van Putten1, Rand Ismaeel1、4, James Williamson5, Katie Addinall5, Daniel Schwendemann6, Martynas Beresna1, Vasilis Apostolopoulos3, and Gilberto Brambilla1
Author Affiliations
  • 1Optoelectronics Research Centre, University of Southampton, Southampton, SO17 1BJ, UK
  • 2School of Physics, Suranaree University of Technology, Nakhon Ratchasima, 30000, Thailand
  • 3School of Physics and Astronomy, University of Southampton, Southampton, SO17 1BJ, UK
  • 4National Oceanography Centre, Southampton, SO14 3ZH, UK
  • 5Centre for Precision Technologies, University of Huddersfield, Huddersfield, HD1 3DH, UK
  • 6Institute for Material Science and Plastics Processing, University of Applied Sciences Eastern Switzerland, Rapperswil, 8640, Switzerland
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    DOI: 10.1364/PRJ.420672 Cite this Article Set citation alerts
    Wanvisa Talataisong, Jon Gorecki, Lieke D. van Putten, Rand Ismaeel, James Williamson, Katie Addinall, Daniel Schwendemann, Martynas Beresna, Vasilis Apostolopoulos, Gilberto Brambilla. Hollow-core antiresonant terahertz fiber-based TOPAS extruded from a 3D printer using a metal 3D printed nozzle[J]. Photonics Research, 2021, 9(8): 1513 Copy Citation Text show less
    (a) Structured nozzle design including a 3D model, a cross section, and various views of the nozzle. (b) Side and bottom views of a metal 3D printed structured nozzle. Cross-section X-ray tomography images of the metal 3D printed nozzle in the (c) x, (d) y, and (e) z planes. Heat transfer simulation of the designed nozzle for applied nozzle thread temperatures of (f) T=300°C and (g) T=220°C.
    Fig. 1. (a) Structured nozzle design including a 3D model, a cross section, and various views of the nozzle. (b) Side and bottom views of a metal 3D printed structured nozzle. Cross-section X-ray tomography images of the metal 3D printed nozzle in the (c) x, (d) y, and (e) z planes. Heat transfer simulation of the designed nozzle for applied nozzle thread temperatures of (f) T=300°C and (g) T=220°C.
    (a) Bottom-view cross section of the nozzle. Yellow represents the area filled by the polymer. (b) Schematic of the cross section of the extruded TOPAS HC fiber.
    Fig. 2. (a) Bottom-view cross section of the nozzle. Yellow represents the area filled by the polymer. (b) Schematic of the cross section of the extruded TOPAS HC fiber.
    (a) Schematic of the experimental setup used to extrude the HC-ARPF from the 3D printer. (b) Photograph and (c) schematic of the HC-ARPF extruded from the heated structured nozzle.
    Fig. 3. (a) Schematic of the experimental setup used to extrude the HC-ARPF from the 3D printer. (b) Photograph and (c) schematic of the HC-ARPF extruded from the heated structured nozzle.
    (a) Cross-section and (b) photograph of the TOPAS hollow-core antiresonant THz fiber extruded from the metal 3D printed structured nozzle. (c) Schematic of the experimental setup used for characterization in the THz regime.
    Fig. 4. (a) Cross-section and (b) photograph of the TOPAS hollow-core antiresonant THz fiber extruded from the metal 3D printed structured nozzle. (c) Schematic of the experimental setup used for characterization in the THz regime.
    (a) Simulation results (COMSOL) for the transmission loss of three HC-ARPFs with different strut thicknesses of 0.55, 0.65, and 0.75 mm. (b) Simulation results for transmission loss of three HC-ARPFs with different core diameters of 2.5, 3.0, and 3.5 mm when the thickness of strut is fixed at 0.65 mm.
    Fig. 5. (a) Simulation results (COMSOL) for the transmission loss of three HC-ARPFs with different strut thicknesses of 0.55, 0.65, and 0.75 mm. (b) Simulation results for transmission loss of three HC-ARPFs with different core diameters of 2.5, 3.0, and 3.5 mm when the thickness of strut is fixed at 0.65 mm.
    Simulated modal profiles in the fiber core at (a) resonant frequency (ν=0.59 THz) and (b) antiresonant frequency (ν=0.70 THz). (c) FEM calculation of the confinement loss of designed HC-ARPF with core diameter d=2.2 mm and thickness of core surround t=0.65 mm.
    Fig. 6. Simulated modal profiles in the fiber core at (a) resonant frequency (ν=0.59THz) and (b) antiresonant frequency (ν=0.70THz). (c) FEM calculation of the confinement loss of designed HC-ARPF with core diameter d=2.2mm and thickness of core surround t=0.65mm.
    (a) Time-domain measurement of the THz wave from THz emitter (collimated beam). (b) Spectral profile of the THz wave from the emitter (black line), when it passes through two THz convex lenses (red line) and when it is transmitted through the HC-ARPF (blue line). (c)–(e) Spectrograms of the THz wave (c) from the THz emitter, (d) after propagating through two THz convex lenses, and (e) through the two convex lenses and a 60 mm long HC-ARPF.
    Fig. 7. (a) Time-domain measurement of the THz wave from THz emitter (collimated beam). (b) Spectral profile of the THz wave from the emitter (black line), when it passes through two THz convex lenses (red line) and when it is transmitted through the HC-ARPF (blue line). (c)–(e) Spectrograms of the THz wave (c) from the THz emitter, (d) after propagating through two THz convex lenses, and (e) through the two convex lenses and a 60 mm long HC-ARPF.
    (a) Spectral profile of the THz waves from the HC-ARPF with the lengths of 40, 60, and 80 mm. Spectrograms of the THz wave from THz HC-ARPF with lengths of (b) 40 mm, (c) 60 mm, and (d) 80 mm. (e) Experimental result and numerical simulation of the loss for the TOPAS HC-ARPF.
    Fig. 8. (a) Spectral profile of the THz waves from the HC-ARPF with the lengths of 40, 60, and 80 mm. Spectrograms of the THz wave from THz HC-ARPF with lengths of (b) 40 mm, (c) 60 mm, and (d) 80 mm. (e) Experimental result and numerical simulation of the loss for the TOPAS HC-ARPF.
    Wanvisa Talataisong, Jon Gorecki, Lieke D. van Putten, Rand Ismaeel, James Williamson, Katie Addinall, Daniel Schwendemann, Martynas Beresna, Vasilis Apostolopoulos, Gilberto Brambilla. Hollow-core antiresonant terahertz fiber-based TOPAS extruded from a 3D printer using a metal 3D printed nozzle[J]. Photonics Research, 2021, 9(8): 1513
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