• Chinese Journal of Lasers
  • Vol. 51, Issue 4, 0402406 (2024)
Zezheng Li1, Shuaipeng Guo1, Chuang Jiang2, Shaolin Ke2, and Zhennan Tian1、*
Author Affiliations
  • 1State Key Laboratory of Integrated Optoelectronics, College of Electronic Science and Engineering, Jilin University, Changchun 130012, Jilin , China
  • 2Hubei Key Laboratory of Optical Information and Pattern Recognition, Wuhan Institute of Technology, Wuhan 430205, Hubei , China
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    DOI: 10.3788/CJL231285 Cite this Article Set citation alerts
    Zezheng Li, Shuaipeng Guo, Chuang Jiang, Shaolin Ke, Zhennan Tian. Three-Dimensional Femtosecond-Laser Direct-Written Optical Waveguide: Advancements and Challenges (Invited)[J]. Chinese Journal of Lasers, 2024, 51(4): 0402406 Copy Citation Text show less
    Three-dimensional optical waveguide devices fabricated by FsLDW technique[5-9]
    Fig. 1. Three-dimensional optical waveguide devices fabricated by FsLDW technique[5-9]
    Schematics of the free electron plasma formation. (a) Multiphoton ionization; (b) tunneling ionization; (c) avalanche ionization
    Fig. 2. Schematics of the free electron plasma formation. (a) Multiphoton ionization; (b) tunneling ionization; (c) avalanche ionization
    Schematics of the cross-section images of waveguides fabricated by FsLDW (the areas within the black dash lines represent the location of waveguide core). (a) Direct-written refractive index elevated waveguide; (b) stress-extruded dual line waveguide; (c) depressed cladding waveguide; (d) ablated ridge waveguide
    Fig. 3. Schematics of the cross-section images of waveguides fabricated by FsLDW (the areas within the black dash lines represent the location of waveguide core). (a) Direct-written refractive index elevated waveguide; (b) stress-extruded dual line waveguide; (c) depressed cladding waveguide; (d) ablated ridge waveguide
    FIFO devices fabricated by FsLDW technique. (a) Sketch of the first FsLDW FIFO device for 4-core fiber[63]; (b) schematic of an FIFO device for 121-core fiber based on a photonic lantern[64]; (c) a fan-out device in optical quantum chips for the observation of N00N state Bloch oscillations[65]; (d) FsLDW prepared FIFO device with board-bandwidth and low insertion loss for 19-core fiber[66]
    Fig. 4. FIFO devices fabricated by FsLDW technique. (a) Sketch of the first FsLDW FIFO device for 4-core fiber[63]; (b) schematic of an FIFO device for 121-core fiber based on a photonic lantern[64]; (c) a fan-out device in optical quantum chips for the observation of N00N state Bloch oscillations[65]; (d) FsLDW prepared FIFO device with board-bandwidth and low insertion loss for 19-core fiber[66]
    Mode controlling devices fabricated by FsLDW technique. (a) Schematic of the first FsLDW OAM beam emitter[75]; (b) schematic of tapered couplers[76]; (c) concept and principle of the trench-based OAM mode multiplexer[5]
    Fig. 5. Mode controlling devices fabricated by FsLDW technique. (a) Schematic of the first FsLDW OAM beam emitter[75]; (b) schematic of tapered couplers[76]; (c) concept and principle of the trench-based OAM mode multiplexer[5]
    1×N splitters fabricated by FsLDW technique. (a) Schematic of the SLM-assisted single-sweep laser direct-written 1×4 splitter[83]; (b) schematic of three-dimensional LiNbO3 splitter based on depressed cladding waveguide[87]; (c)(d) schematic of splitter with the optical-lattice-like cladding and its output modal profile[88]
    Fig. 6. N splitters fabricated by FsLDW technique. (a) Schematic of the SLM-assisted single-sweep laser direct-written 1×4 splitter[83]; (b) schematic of three-dimensional LiNbO3 splitter based on depressed cladding waveguide[87]; (c)(d) schematic of splitter with the optical-lattice-like cladding and its output modal profile[88]
    Three-dimensional quantum photonic chips fabricated by FsLDW technique. (a) Schematic of the first three qubit quantum Toffoli gate[96]; (b) three-dimensional waveguide array for the two-mode braiding[6]; (c) the array with 2401 waveguides for two-dimensional quantum walks[98]; (d) three-waveguide coupled system introducing the birefringence[99]; (e) schematics for four-mode and eight-mode integrated interferometers for the implementation of qFFT[100]; (f) schematic of a glued hexagonal tree[101]
    Fig. 7. Three-dimensional quantum photonic chips fabricated by FsLDW technique. (a) Schematic of the first three qubit quantum Toffoli gate[96]; (b) three-dimensional waveguide array for the two-mode braiding[6]; (c) the array with 2401 waveguides for two-dimensional quantum walks[98]; (d) three-waveguide coupled system introducing the birefringence[99]; (e) schematics for four-mode and eight-mode integrated interferometers for the implementation of qFFT[100]; (f) schematic of a glued hexagonal tree[101]
    Topological phase in optical waveguide arrays. (a) Spiral induced Floquet topological insulator[7]; (b) bulk band structure of Floquet topological insulators[7]; (c)(d) optical field distributions on the output surface of the waveguide array at different propagation distances[7]; (e) one-dimensional non-Hermitian SSH model[104]; (f) experimental and simulation results of mean displacement〈Δm〉for different distance differences Δd between waveguids[104]; (g) nonlinear induced photon anomalous Floquet topological insulator[105]; (h) bulk band structure of anomalous Floquet topological insulators[105]; (i) light diffraction in the anomalous Floquet arrays under linear and nonlinear edge excitation regimes[105]
    Fig. 8. Topological phase in optical waveguide arrays. (a) Spiral induced Floquet topological insulator[7]; (b) bulk band structure of Floquet topological insulators[7]; (c)(d) optical field distributions on the output surface of the waveguide array at different propagation distances[7]; (e) one-dimensional non-Hermitian SSH model[104]; (f) experimental and simulation results of mean displacement〈Δm〉for different distance differences Δd between waveguids[104]; (g) nonlinear induced photon anomalous Floquet topological insulator[105]; (h) bulk band structure of anomalous Floquet topological insulators[105]; (i) light diffraction in the anomalous Floquet arrays under linear and nonlinear edge excitation regimes[105]
    Three-dimensional optical waveguide devices for astrophotonics. (a) Schematic of the PL with Bragg gratings[110]; (b) schematic of the photonic dicer[8]; (c) schematic of the pupil remapper[111]; (d) schematic of three-dimensional beam combiner[112]
    Fig. 9. Three-dimensional optical waveguide devices for astrophotonics. (a) Schematic of the PL with Bragg gratings[110]; (b) schematic of the photonic dicer[8]; (c) schematic of the pupil remapper[111]; (d) schematic of three-dimensional beam combiner[112]
    Three-dimensional waveguide sensors. (a) Schematic of the femtosecond-laser-fabricated microfluidic channel and integrated MZI[117]; (b)(c) schematic of the RI sensor in silver containing glasses and transmission curves of the sensor under different refractive index oils[118]; (d) schematic of the cascaded FPI and MZI sensing structure[121]; (e) schematic of an HBGW created in coreless fiber[122]
    Fig. 10. Three-dimensional waveguide sensors. (a) Schematic of the femtosecond-laser-fabricated microfluidic channel and integrated MZI[117]; (b)(c) schematic of the RI sensor in silver containing glasses and transmission curves of the sensor under different refractive index oils[118]; (d) schematic of the cascaded FPI and MZI sensing structure[121]; (e) schematic of an HBGW created in coreless fiber[122]
    Spherical aberration and its compensation techniques. (a) Introduction of spherical aberration[138]; (b) schematic of the slit shaping optical path[145]; (c) optical microscopy photo of the circular cross-section optical waveguide written by the cylindrical lens and slit combination optical path and the scale bar is 10 μm[146]; (d) deep structures direct writing with the aid of SLM compensation algorithm[148]; (e) schematic of the multi-foci-shaped femtosecond laser direct writing optical path[150]
    Fig. 11. Spherical aberration and its compensation techniques. (a) Introduction of spherical aberration[138]; (b) schematic of the slit shaping optical path[145]; (c) optical microscopy photo of the circular cross-section optical waveguide written by the cylindrical lens and slit combination optical path and the scale bar is 10 μm[146]; (d) deep structures direct writing with the aid of SLM compensation algorithm[148]; (e) schematic of the multi-foci-shaped femtosecond laser direct writing optical path[150]
    Direct writing of large-depth waveguides by compensating the spherical aberration by SLM. (a) Symmetric cross-sections of waveguides written under different deptths[152]; (b) large-scale uniform waveguide array for achieving structural invisibility[153]
    Fig. 12. Direct writing of large-depth waveguides by compensating the spherical aberration by SLM. (a) Symmetric cross-sections of waveguides written under different deptths[152]; (b) large-scale uniform waveguide array for achieving structural invisibility[153]
    Three-dimensional reconfigurable optical waveguides. (a) Depth-varying overpass waveguides[157]; (b) waveguide in a cantilever beam[158]
    Fig. 13. Three-dimensional reconfigurable optical waveguides. (a) Depth-varying overpass waveguides[157]; (b) waveguide in a cantilever beam[158]
    SubstrateRepetition rate /kHzScanning velocity /(mm·s-1Guiding wavelength /nmPropagation loss /(dB·cm-1Ref.
    Fused silica5000.12515500.07123
    Eagle XG500115500.26125
    BK710001.515500.3124
    Lead-germanate glass50000.515500.2126
    BZH72500.215500.2127
    Chalcogenide glass600115500.15128
    Nd∶YVO410.510640.46130
    Diamond10.16331.2131
    Z-LiNbO311015500.4132
    β-BBO10.58000.19129
    Pr∶YLF10.054440.12133
    YAG∶Nd10.510640.15134
    PMMA100368500.5135
    Table 1. Low-loss waveguides in various substrates fabricated by FsLDW technology
    Zezheng Li, Shuaipeng Guo, Chuang Jiang, Shaolin Ke, Zhennan Tian. Three-Dimensional Femtosecond-Laser Direct-Written Optical Waveguide: Advancements and Challenges (Invited)[J]. Chinese Journal of Lasers, 2024, 51(4): 0402406
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