• Photonics Research
  • Vol. 9, Issue 7, 1182 (2021)
Ahmed E. Hassanien*, Steffen Link, Yansong Yang, Edmond Chow, Lynford L. Goddard, and Songbin Gong
Author Affiliations
  • Holonyak Micro and Nanotechnology Laboratory, Department of Electrical and Computer Engineering, University of Illinois at Urbana-Champaign, Urbana, Illinois 61801, USA
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    DOI: 10.1364/PRJ.421612 Cite this Article Set citation alerts
    Ahmed E. Hassanien, Steffen Link, Yansong Yang, Edmond Chow, Lynford L. Goddard, Songbin Gong. Efficient and wideband acousto-optic modulation on thin-film lithium niobate for microwave-to-photonic conversion[J]. Photonics Research, 2021, 9(7): 1182 Copy Citation Text show less

    Abstract

    Microwave photonics, a field that crosscuts microwave/millimeter-wave engineering with optoelectronics, has sparked great interest from research and commercial sectors. This multidisciplinary fusion can achieve ultrawide bandwidth and ultrafast speed that were considered impossible in conventional chip-scale microwave/millimeter-wave systems. Conventional microwave-to-photonic converters, based on resonant acousto-optic modulation, produce highly efficient modulation but sacrifice bandwidth and limit their applicability for most real-world microwave signal-processing applications. In this paper, we build highly efficient and wideband microwave-to-photonic modulators using the acousto-optic effect on suspended lithium niobate thin films. A wideband microwave signal is first piezoelectrically transduced using interdigitated electrodes into Lamb acoustic waves, which directly propagates across an optical waveguide and causes refractive index perturbation through the photoelastic effect. This approach is power-efficient, with phase shifts up to 0.0166 rad/mW over a 45 μm modulation length and with a bandwidth up to 140 MHz at a center frequency of 1.9 GHz. Compared to the state-of-the-art, a 9× more efficient modulation has been achieved by optimizing the acoustic and optical modes and their interactions.
    Δnn=12ne2(P32δ2+P33δ3),

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    Δφn=2πΔnLmodλmod,

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    ΔφL=2πnΔLλmod,

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    P0opt=PinoptT2[1+J0(|Δφn|)cos(ΔφL)],

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    P1opt=PinoptTJ1(|Δφn|)sin(ΔφL),

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    P0RF=C4×[1+J0(|Δφn|)×cos(ΔφL)]2,

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    P1RF=C×[J1(|Δφn|)×sin(ΔφL)]2,

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    C=(PinoptTGPR)22×50,

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    Vπ=P0opt×GPR×π|S21|,

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    Eout,m=Ein2ejβmLmtm,(A1)

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    Poutopt=PinoptT2[1+cos(β1L1β2L2)].(A2)

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    β1L1β2L2=2πnLunmodλ+2π(n+Δn)Lmodλ2πn(Lunmod+Lmod+ΔL)λ=2πΔnLmodλ2πnΔLλ.(A3)

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    Δφn=2πΔnLmodλ,(A4)

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    ΔφL=2πnΔLλ,(A5)

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    Poutopt=PinoptT2{1+cos[|Δφn|cos(ωRFt)]cos(ΔφL)+sin[|Δφn|cos(ωRFt)]sin(ΔφL)},(A6)

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    cos(xcosθ)=J0(x)+2m=1(1)mJ2m(x)cos(2mθ),(A7)

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    sin(xcosθ)=2m=1(1)mJ2m1(x)cos[(2m1)θ].(A8)

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    Poutopt=PinoptT2{1+[J0(|Δφn|)+2m=1(1)mJ2m(|Δφn|)cos(2mωRFt)]cos(ΔφL)+{2m=1(1)mJ2m1(|Δφn|)cos[(2m1)ωRFt]}sin(ΔφL)}.(A9)

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    P0opt=PinoptT2[1+J0(|Δφn|)cos(ΔφL)],(A10)

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    P1opt=PinoptTJ1(|Δφn|)sin(ΔφL),(A11)

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    P2opt=PinoptTJ2(|Δφn|)cos(ΔφL),(A12)

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    P3opt=PinoptTJ3(|Δφn|)sin(ΔφL).(A13)

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    PoutRF=(PoutoptGPR)22×50,(A14)

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    P0RF=C4[1+J0(|Δφn|)cos(ΔφL)]2,(A15)

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    P1RF=C[J1(|Δφn|)sin(ΔφL)]2,(A16)

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    P2RF=C[J2(|Δφn|)cos(ΔφL)]2,(A17)

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    P3RF=C[J3(|Δφn|)sin(ΔφL)]2,(A18)

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    C=(Pinopt×T×GPR)22×50.(A19)

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    P1RF=P0RFΔφn2=(P0optGPR)22×50(πVVπ)2=PinRF(P0optGPRπVπ)2.(B1)

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    Vπ=P0optGPRπ|S21|.(B2)

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    PIDTπRF=PinπRF(1|S11|2),(B3)

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    PinπRF=Vπ22×50.(B4)

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    ap=πPIDTπ.(B5)

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    [1no2+Δ(1n12)]x2+[1no2+Δ(1n22)]y2+[1ne2+Δ(1n32)]z2+[2Δ(1n42)]yz+[2Δ(1n52)]xz+[2Δ(1n62)]xy=1,(C1)

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    Δnn=12ne2Δ(1n32),(C2)

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    Δ(1ni2)=Pijδj,(C3)

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    [0.0450.0960.1490.055000.0960.0450.1490.055000.1380.1380.0760000.120.1200.0190000000.0190.1200000.0550.025].(C4)

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    Δ(1ni2)=rijEj,(C5)

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    r=[03.48.603.48.60030.8028028003.400]pm/V.(C6)

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    Δnn=12ne2(P32δ2+P33δ3),(C7)

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    Δnn=12ne2(r33E3).(C8)

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    Ahmed E. Hassanien, Steffen Link, Yansong Yang, Edmond Chow, Lynford L. Goddard, Songbin Gong. Efficient and wideband acousto-optic modulation on thin-film lithium niobate for microwave-to-photonic conversion[J]. Photonics Research, 2021, 9(7): 1182
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