Author Affiliations
1State Key Laboratory of Integrated Optoelectronics, College of Electronic Science and Engineering, Jilin University, Changchun 130012, Jilin , China2Hubei Key Laboratory of Optical Information and Pattern Recognition, Wuhan Institute of Technology, Wuhan 430205, Hubei , Chinashow less
Fig. 1. Three-dimensional optical waveguide devices fabricated by FsLDW technique
[5-9] Fig. 2. Schematics of the free electron plasma formation. (a) Multiphoton ionization; (b) tunneling ionization; (c) avalanche ionization
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
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] 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] Fig. 6. 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 LiNbO
3 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. 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] 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〈Δ
m〉for different distance differences Δ
d 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. 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] 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] 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] 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] Fig. 13. Three-dimensional reconfigurable optical waveguides. (a) Depth-varying overpass waveguides
[157]; (b) waveguide in a cantilever beam
[158] Substrate | Repetition rate /kHz | Scanning velocity /(mm·s-1) | Guiding wavelength /nm | Propagation loss /(dB·cm-1) | Ref. |
---|
Fused silica | 500 | 0.125 | 1550 | 0.07 | [123] | Eagle XG | 500 | 1 | 1550 | 0.26 | [125] | BK7 | 1000 | 1.5 | 1550 | 0.3 | [124] | Lead-germanate glass | 5000 | 0.5 | 1550 | 0.2 | [126] | BZH7 | 250 | 0.2 | 1550 | 0.2 | [127] | Chalcogenide glass | 600 | 1 | 1550 | 0.15 | [128] | Nd∶YVO4 | 1 | 0.5 | 1064 | 0.46 | [130] | Diamond | 1 | 0.1 | 633 | 1.2 | [131] | Z-LiNbO3 | 1 | 10 | 1550 | 0.4 | [132] | β-BBO | 1 | 0.5 | 800 | 0.19 | [129] | Pr∶YLF | 1 | 0.05 | 444 | 0.12 | [133] | YAG∶Nd | 1 | 0.5 | 1064 | 0.15 | [134] | PMMA | 100 | 36 | 850 | 0.5 | [135] |
|
Table 1. Low-loss waveguides in various substrates fabricated by FsLDW technology