• Acta Optica Sinica
  • Vol. 42, Issue 23, 2313001 (2022)
Bin Zhang1、2、* and Zhaohui Li1、2、3
Author Affiliations
  • 1Guangdong Provincial Key Laboratory of Optoelectronic Information Processing Chips and Systems, School of Electronics and Information Technology, Sun Yat-Sen University, Guangzhou 510275, Guangdong , China
  • 2State Key Laboratory of Optoelectronic Materials and Technologies, Sun Yat-Sen University, Guangzhou 510275, Guangdong , China
  • 3Southern Marine Science and Engineering Guangdong Laboratory (Zhuhai), Zhuhai 519000, Guangdong , China
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    DOI: 10.3788/AOS202242.2313001 Cite this Article Set citation alerts
    Bin Zhang, Zhaohui Li. Integrated Chalcogenide Photonics[J]. Acta Optica Sinica, 2022, 42(23): 2313001 Copy Citation Text show less
    Infrared transmission window of some materials[25-29]
    Fig. 1. Infrared transmission window of some materials[25-29]
    Surface topographies of ChG films deposited by different methods. (a) AFM image of GeAsSe films deposited by magnetron sputtering[69]; (b) optical microscopy image of Ge2Sb2Te5 thin film deposited by fs-PLD[65]; (c) AFM image of As33S67 film fabricated by sol-gel process[70]; (d) As2S3 films deposited on SiO2 microdisks by thermal evaporation[66]; (e) 4 inch Ge25Sb10S65 film fabricated by thermal evaporation[67]; (f) As55S45 film fabricated by PECVD[68]
    Fig. 2. Surface topographies of ChG films deposited by different methods. (a) AFM image of GeAsSe films deposited by magnetron sputtering[69]; (b) optical microscopy image of Ge2Sb2Te5 thin film deposited by fs-PLD[65]; (c) AFM image of As33S67 film fabricated by sol-gel process[70]; (d) As2S3 films deposited on SiO2 microdisks by thermal evaporation[66]; (e) 4 inch Ge25Sb10S65 film fabricated by thermal evaporation[67]; (f) As55S45 film fabricated by PECVD[68]
    Morphology images of ChG waveguides obtained by different waveguide fabrication methods. (a) SEM images of Ge22As20Se58 waveguide fabricated by direct laser writing[71]; (b) schematic of 80GeS2-15Ga2S3-5Sb2S3 waveguide fabricated by He+ ions implanting[85]; (c) SEM images of As2S3 waveguide fabricated by thermal printing[76]; (d) SEM image of As2Se3 waveguide fabricated by wet-etching[86]; (e) AFM image of Ge23Sb7S70 waveguide fabricated by lift-off [80]
    Fig. 3. Morphology images of ChG waveguides obtained by different waveguide fabrication methods. (a) SEM images of Ge22As20Se58 waveguide fabricated by direct laser writing[71]; (b) schematic of 80GeS2-15Ga2S3-5Sb2S3 waveguide fabricated by He+ ions implanting[85]; (c) SEM images of As2S3 waveguide fabricated by thermal printing[76]; (d) SEM image of As2Se3 waveguide fabricated by wet-etching[86]; (e) AFM image of Ge23Sb7S70 waveguide fabricated by lift-off [80]
    Morphology images of ChG waveguides fabricated by dry-etching method. (a) Schematic of As2S3 waveguide pre-patterned and redeposited on SiO2 substrate[66]; (b) SEM image of Ge23Sb7S70 waveguide prepared with SF6 as etching gas[91]; (c) SEM image of Ge23Sb7S70 waveguide prepared with chlorine as etching gas[92]; (d) SEM image of Ge23Sb7S70 waveguide prepared with CHF3/CF4 as etching gas[93]; (e) SEM image of As2S3 waveguide prepared with CF4/O2 as etching gas[94]; (f) SEM images of Ge25Sb10S65 waveguide sidewall prepared with and without optimized parameters of Ar/CHF3/CF4/O2[53]
    Fig. 4. Morphology images of ChG waveguides fabricated by dry-etching method. (a) Schematic of As2S3 waveguide pre-patterned and redeposited on SiO2 substrate[66]; (b) SEM image of Ge23Sb7S70 waveguide prepared with SF6 as etching gas[91]; (c) SEM image of Ge23Sb7S70 waveguide prepared with chlorine as etching gas[92]; (d) SEM image of Ge23Sb7S70 waveguide prepared with CHF3/CF4 as etching gas[93]; (e) SEM image of As2S3 waveguide prepared with CF4/O2 as etching gas[94]; (f) SEM images of Ge25Sb10S65 waveguide sidewall prepared with and without optimized parameters of Ar/CHF3/CF4/O2[53]
    Applications of integrated ChG devices in ultrabroad wavelength regions. (a) Narrow bandwidth Bragg grating filter based on chalcogenide glass in 1.55 μm band[109]; (b) graphene waveguide integrated detector in 2 μm band[115]; (c) schematic of photon aerosol spectrometer module in 3 μm band[116]; (d) schematic of hybrid integrated detector based on spiral chalcogenide waveguide and PbTe film directly integrated under chalcogenide waveguide[112]; (e) cross-section structure and (f) transmission spectrum of As2Se3 waveguides in mid-infrared band[83]; (g) optical microscope image of spiral single-mode ChG waveguide detector and (h) absorption spectra of methane and nitrous oxide based on device in 7-9 μm wavelength region[117]
    Fig. 5. Applications of integrated ChG devices in ultrabroad wavelength regions. (a) Narrow bandwidth Bragg grating filter based on chalcogenide glass in 1.55 μm band[109]; (b) graphene waveguide integrated detector in 2 μm band[115]; (c) schematic of photon aerosol spectrometer module in 3 μm band[116]; (d) schematic of hybrid integrated detector based on spiral chalcogenide waveguide and PbTe film directly integrated under chalcogenide waveguide[112]; (e) cross-section structure and (f) transmission spectrum of As2Se3 waveguides in mid-infrared band[83]; (g) optical microscope image of spiral single-mode ChG waveguide detector and (h) absorption spectra of methane and nitrous oxide based on device in 7-9 μm wavelength region[117]
    Applications of ChG phase change material-based photonic integrated devices. (a) Optical switch based on Si3N4 microresonator and GST[118]; (b) 1×2 and 2×2 phase change material-based optical switchs[122]; (c) GSST based polarization rotary optical switch[125]; (d) working principle and multi-level signal processing of all-optical on-chip memory device[127]; (e) GST based photonic memory cell and photonic structure of matrix-vector multiplication[128]; (f) photonic tensor cores for convolution operations[8]; (g) optical switches based on symmetric and asymmetric microring resonators[129]
    Fig. 6. Applications of ChG phase change material-based photonic integrated devices. (a) Optical switch based on Si3N4 microresonator and GST[118]; (b) 1×2 and 2×2 phase change material-based optical switchs[122]; (c) GSST based polarization rotary optical switch[125]; (d) working principle and multi-level signal processing of all-optical on-chip memory device[127]; (e) GST based photonic memory cell and photonic structure of matrix-vector multiplication[128]; (f) photonic tensor cores for convolution operations[8]; (g) optical switches based on symmetric and asymmetric microring resonators[129]
    Results of ChG optical waveguides fabricated by laser direct writing method[132]. Optical microscope images of (a) unexposed area, (b) single straight waveguide, and (c) Y-coupler on ChG film; (d) top view of microring resonator obtained by optical microscope[133]; (e) fabrication schematic of optical Bragg grating through interference caused by dislocation of shadow masks[134]
    Fig. 7. Results of ChG optical waveguides fabricated by laser direct writing method[132]. Optical microscope images of (a) unexposed area, (b) single straight waveguide, and (c) Y-coupler on ChG film; (d) top view of microring resonator obtained by optical microscope[133]; (e) fabrication schematic of optical Bragg grating through interference caused by dislocation of shadow masks[134]
    Results of mode splitting caused by photorefractive in ChG microresonators[136]. (a) Optical microscope image of ChG microresonator; (b) schematic of Bragg grating in ChG microresonator; (c) pattern splitting results caused by different irradiation time; (d) variation curves of mode splitting width Δλsplit and corresponding Bragg grating reflectivity rB with exposure time; (e) reflection spectra of "writing" and "erasing" selected mode in As2S3 microcavity based on photoinduced refractive index variation[137] (upper image is reflection spectrum including three modes, lower left image is reflection spectrum of three modes after erasing mode 2, lower middle image is local reflection spectrum before erasing mode 2, and lower right image is local reflection spectrum after erasing mode 2)
    Fig. 8. Results of mode splitting caused by photorefractive in ChG microresonators[136]. (a) Optical microscope image of ChG microresonator; (b) schematic of Bragg grating in ChG microresonator; (c) pattern splitting results caused by different irradiation time; (d) variation curves of mode splitting width Δλsplit and corresponding Bragg grating reflectivity rB with exposure time; (e) reflection spectra of "writing" and "erasing" selected mode in As2S3 microcavity based on photoinduced refractive index variation[137] (upper image is reflection spectrum including three modes, lower left image is reflection spectrum of three modes after erasing mode 2, lower middle image is local reflection spectrum before erasing mode 2, and lower right image is local reflection spectrum after erasing mode 2)
    Hybrid integrated ChG-based devices. (a) ChG and lithium niobate hybrid integrated microring modulator and MZI modulator[139]; (b) As2S3 vertically integrated optical phased array on lithium niobate substrate[141]; (c) acoustooptic modulator with lithium niobate/GeSbS hybrid integrated MZI structure[144]; (d) GeSbSe waveguide integrated black phosphorus photodetector[147]; (e) hybrid integrated photodetector based on ChG waveguide and tellurene[148]
    Fig. 9. Hybrid integrated ChG-based devices. (a) ChG and lithium niobate hybrid integrated microring modulator and MZI modulator[139]; (b) As2S3 vertically integrated optical phased array on lithium niobate substrate[141]; (c) acoustooptic modulator with lithium niobate/GeSbS hybrid integrated MZI structure[144]; (d) GeSbSe waveguide integrated black phosphorus photodetector[147]; (e) hybrid integrated photodetector based on ChG waveguide and tellurene[148]
    ChG waveguides and systems for all-optical signal processing[154]. (a) Cross section of As2S3 planar waveguide; (b) simulated group velocity dispersion of TE and TM modes and material dispersion of on-chip waveguide; (c) principle diagrams of transmitter optimization of Tbit/s bandwidth signal and demultiplexing time division multiplexing signal receiver system
    Fig. 10. ChG waveguides and systems for all-optical signal processing[154]. (a) Cross section of As2S3 planar waveguide; (b) simulated group velocity dispersion of TE and TM modes and material dispersion of on-chip waveguide; (c) principle diagrams of transmitter optimization of Tbit/s bandwidth signal and demultiplexing time division multiplexing signal receiver system
    Results of ChG integrated microresonators in optical parametric oscillation applications. (a) Optical parametric oscillation based on As2S3 microring resonators[30];(b) measured threshold power of optical parametric oscillation process (about 5.4 mW)[30]; (c) four-wave mixing effect based on Ge11.5As24Se64.5 microring resonators[158]; (d) measured conversion efficiency of four wave mixing as a function of input pump power[158]
    Fig. 11. Results of ChG integrated microresonators in optical parametric oscillation applications. (a) Optical parametric oscillation based on As2S3 microring resonators[30];(b) measured threshold power of optical parametric oscillation process (about 5.4 mW)[30]; (c) four-wave mixing effect based on Ge11.5As24Se64.5 microring resonators[158]; (d) measured conversion efficiency of four wave mixing as a function of input pump power[158]
    Results of ChG integrated microresonators in optical frequency comb applications[53,67]. (a) SEM of GeSbS microresonator;(b) bright soliton microcomb; (c) dark-pulse microcomb; (d) Raman-Kerr microcomb
    Fig. 12. Results of ChG integrated microresonators in optical frequency comb applications[53,67]. (a) SEM of GeSbS microresonator;(b) bright soliton microcomb; (c) dark-pulse microcomb; (d) Raman-Kerr microcomb
    Results of ChG integrated waveguides in SBS applications. (a) SEM of As2S3 rib waveguide; (b) 52 dB Brillouin on-off gain spectrum of As2S3 rib waveguide[164]; (c)(d) As2S3-silicon hybrid integrated waveguide and its Brillouin gain spectrum[165]; (e)(f) As2S3-Ge∶SiO2 hybrid integrated waveguides and its Brillouin gain spectrum[167]; (g)(h) Ge25Sb10S65 waveguides and its Brillouin gain spectrum[168]; (i)(j) As2S3 waveguides with BCB cladding and its Brillouin gain spectrum[169]
    Fig. 13. Results of ChG integrated waveguides in SBS applications. (a) SEM of As2S3 rib waveguide; (b) 52 dB Brillouin on-off gain spectrum of As2S3 rib waveguide[164]; (c)(d) As2S3-silicon hybrid integrated waveguide and its Brillouin gain spectrum[165]; (e)(f) As2S3-Ge∶SiO2 hybrid integrated waveguides and its Brillouin gain spectrum[167]; (g)(h) Ge25Sb10S65 waveguides and its Brillouin gain spectrum[168]; (i)(j) As2S3 waveguides with BCB cladding and its Brillouin gain spectrum[169]
    Applications of SBS in ChG integrated chips. (a) Microwave photonics filters[171-174]; (b) low-noise microwave source[175]; (c) microwave measurement[176]; (d) narrow linewidth on-chip Brillouin laser[66,165] ; (e) high spatial resolution sensing[177]; (f) photonic memory[179]
    Fig. 14. Applications of SBS in ChG integrated chips. (a) Microwave photonics filters[171-174]; (b) low-noise microwave source[175]; (c) microwave measurement[176]; (d) narrow linewidth on-chip Brillouin laser[66,165] ; (e) high spatial resolution sensing[177]; (f) photonic memory[179]
    Large bandwidth tunable ChG-based integrated Raman laser[53]. (a) SEM of GeSbS microresonator; (b) Raman laser spectrum; (c) output power of the first-order Raman laser as a function of pump power; (d)(e) discrete tuning of the first Stokes output spectrum and discrete tuning of power; (f) discrete tuning of second-order Stokes output spectrum; (g) continuous tuning of Raman laser at different temperatures
    Fig. 15. Large bandwidth tunable ChG-based integrated Raman laser[53]. (a) SEM of GeSbS microresonator; (b) Raman laser spectrum; (c) output power of the first-order Raman laser as a function of pump power; (d)(e) discrete tuning of the first Stokes output spectrum and discrete tuning of power; (f) discrete tuning of second-order Stokes output spectrum; (g) continuous tuning of Raman laser at different temperatures
    Integrated Raman soliton laser based on ChG waveguides[182]. (a) Optical microscope image and SEM image of fabricated device with varying waveguide width between 800 and 1000 nm; (b) diagram of experimental setup; (c) measured optical spectra of Raman solitons; (d) Raman soliton spectrum under 7.73 pJ pulse energy; (e) Raman soliton pulse train; (f) autocorrelation trace of Raman soliton single pulse; (g) frequency domain analysis of Raman soliton
    Fig. 16. Integrated Raman soliton laser based on ChG waveguides[182]. (a) Optical microscope image and SEM image of fabricated device with varying waveguide width between 800 and 1000 nm; (b) diagram of experimental setup; (c) measured optical spectra of Raman solitons; (d) Raman soliton spectrum under 7.73 pJ pulse energy; (e) Raman soliton pulse train; (f) autocorrelation trace of Raman soliton single pulse; (g) frequency domain analysis of Raman soliton
    MaterialGeometryn2 /(10-18 m2·W-1Loss /(dB·cm-1Qint /106TPA /(m·W-1
    As2S330Waveguide30.1Negligible
    Ge11.5As24Se64.531Waveguide8.62.610-13
    Ge22Sb18Se6032Waveguide5.144×10-13
    Si33Waveguide645×10-12
    AlGaAs34-36Waveguide14.33.25×10-12
    LiNbO337Microring0.18~4Negligible
    SiC38Microdisk0.87.1Negligible
    Si3N439-40Microring0.25422Negligible
    AlN41Microring~0.351.1Negligible
    GaN42Microring1.40.241.8Negligible
    GaP43Microring111.22Negligible
    Table 1. Nonlinear optical parameters of some materials at 1.55 μm

    Material

    type

    Fabrication

    method

    Refractive indexDimensionLoss or Q factor

    Ge23Sb7S70

    waveguide96

    TE

    RIE

    2.18

    0.8 μm(width)×

    0.42 μm(height)

    0.5 dB·cm-1

    Ge23Sb7S70

    microdisk93

    TE

    RIE

    2.220.8 μm×0.45 μm1.2×106
    Ge11.5As24Se64.5 nanowires31

    TE

    ICP(inductive coupled plasma)-RIE

    2.660.63 μm×0.5 μm2.6 dB·cm-1

    Ge11.5As24Se64.5

    microdisk97

    TE

    RIE

    2.5451 μm height1.1×106

    Ge25Sb10S65

    microring67

    TE

    ICP-RIE

    2.22.4 μm×0.8 μm1.3×106

    Ge28Sb12Se60

    microdisk98

    TE

    ICP

    2.81 μm height5 ×105

    Ge28Sb12Se60

    microring99

    TE

    ICP

    2.80.3 μm height4.1 ×105

    As20S80

    resonator88

    Micro-trench

    EBE(electron beam evaporator)

    2.16582.0 μm×1.5 μm6×105

    As2S3

    resonator66

    Trapezoidal-

    TE

    2.4310 µm×1.3 µm1.44×107

    As2S3

    microring100

    Micro-trench

    TE

    2.452.5 μm×1.4 µm4.6×105
    Table 2. Parameters of chalcogenide optical waveguide and microresonator at 1.55 µm
    Wavelength /μm

    Material

    type

    Fabrication

    method

    Refractive indexDimensionLoss or Q factor
    3.8-5

    Ge11.5As24Se64.5

    waveguide101

    TE

    ICP

    4.0 μm(width)×4.4 μm(height)~0.6 dB·cm-1
    5.2

    Ge23Sb7S70

    microdisk102

    TE

    Lift-off

    ~2.13 µm×1.3 µm4×105
    2.5-6.6

    Ge11.5As24Se64.5

    waveguide103

    TE

    ICP

    2.6094 µm×1.25 µm~0.5 dB·cm-1
    2

    As2S3

    waveguide104

    TE

    ICP

    2.421.2 μm×0.6 µm1.45 dB·cm-1
    5.2

    As2S3

    microdisk83

    TE

    Lift-off

    2.662.5 μm×1.1 μm2×105
    2.4

    As2Se3

    waveguide105

    Sputtering

    Lift-off

    2.7910 μm×1 μm0.16 dB·cm-1
    8.4

    As2Se3

    waveguide71

    TE

    Wet etching

    2.785.4 μm×4.53 μm0.5 dB·cm-1
    Table 3. Parameters of chalcogenide optical waveguide and microresonator in mid-infrared band
    MaterialLength /cm

    Loss /

    (dB·cm-1

    Brillouin

    frequency /GHz

    Gain,

    GB /(m-1·W-1

    Pump power /mWOn/off gain /dB
    As2S316370.47.7310.8730018.8
    As2S317070.47.7317.3930025.8
    As2S3164230.57.650035052
    As2S3-Si1655.80.77.675018022.5
    As2S3-Ge∶SiO2167230.57.8419158~23
    Ge25Sb10S6516870.27.44333820017.6
    aAs2S3-Si1660.817.585280100-
    As2S3-BCB1697.50.27.751711205.95
    Table 4. Comparison of Brillouin gain characteristics of integrated chalcogenide waveguides