• Acta Photonica Sinica
  • Vol. 50, Issue 5, 139 (2021)
Guifa WANG1、2, Mengyue GUO1、2, Jiamei GU1、2, Min TANG1、2, Zhengjun WEI1、2, Jindong WANG1、2, and Shentao WANG3
Author Affiliations
  • 1Guangdong Provincial Key Laboratory of Quantum Engineering and Quantum Materials, South China Normal University, Guangzhou50006, China
  • 2Guangdong Provincial Key Laboratory of Nanophotonic Functional Materials and Devices, South China Normal University, Guangzhou510006, China
  • 3Communication NCO Academy, Peoples Liberation Army Engineering University, Chongqing400056,China
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    DOI: 10.3788/gzxb20215005.0506004 Cite this Article
    Guifa WANG, Mengyue GUO, Jiamei GU, Min TANG, Zhengjun WEI, Jindong WANG, Shentao WANG. Low Power Consumption Visible Light Communication Technology Based on Bilevel Pulse Width Modulation[J]. Acta Photonica Sinica, 2021, 50(5): 139 Copy Citation Text show less

    Abstract

    pulse width modulation technology is proposed. Bilevel pulse width modulation is analyzed in terms of bandwidth requirement, junction capacitance and error performance, and compared with non return to zero on key modulation, pulse position modulation and digital pulse interval modulation.The results show that the two-level pulse width modulation and the non-return-to-zero on-off keying modulation have the same time slot error rate, but the additional power consumption is only M/2 of the non-return-to-zero on-off keying modulation, and M is the modulation order. Although the bilevel pulse width modulation requires higher signal-to-noise ratio compared with pulse position modulation and digital pulse interval modulation, the additional power consumption is only half of that of pulse position modulation and digital pulse interval modulation, and the bandwidth requirement is also less than that of pulse position modulation and digital pulse interval modulation, it has great advantages in power and bandwidth sensitive visible light communication system.
    Jrise=0Tric·vRdt=0Tric·(K1VH-vLED)dt(1)

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    ic=CLED·dvLEDdt(2)

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    Jrise=VLVHK1VH-vLED·CLEDdv=CLEDK1VH-12vL-12vH·vH-vL(3)

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    Jfall=0TfiR·vRdt=0TfiR·(vLED-K2VL)dt=0Tf(iC-iD)·(vLED-K2VL)dt(4)

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    iD=IS(evLEDnVT-1)(5)

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    Jfall=12CLED·(VH-K2VL)2-VHK2VLCLED·(RO+RS)IS(eVLEDnVT-1)·(vLED-K2VL)(RO+RS)IS(eVLEDnVT-1)+vLED-K2VLdvLED(6)

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    Jfall=12CLED·(VH-K2VL)2(7)

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    W=12·f·CLEDK1VH-12VL-12VH·(VH-VL)+14·f·CLED·(VH-K2VL)2         VH>K2VLW=12·f·CLEDK1VH-12VL-12VH·(VH-VL)                                                                   VH<K2VL(8)

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    W=12·f·CLEDK1VH-12VL-12VH·(VH-VL)+14·f·CLED·( VH-K2VL)2         VH>K2VLW=12·f·CLEDK1VH-12VL-12VH·(VH-VL)                                                                   VH<K2VL(9)

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    W=f2M·CLEDK1VH-12VL-12VH·(VH-VL)+f2M·CLED·(VH-K2VL)2            VH>K2VLW=f2M·CLEDK1VH-12VL-12VH·(VH-VL)                                                                    VH<K2VL(10)

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    W=fM·CLEDK1VH-12VL-12VH·(VH-VL)+fM·CLED·(VH-K2VL)2            VH>K2VLW=fM·CLEDK1VH-12VL-12VH·(VH-VL)                                                                 VH<K2VL(11)

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    Pe0=kEr+12πσexp-y22σ2dy=QkErσPe1=-kEr12πσexp-(y-Er)22σ2dy=Q(1-k)Erσ(12)

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    Q(x)=x+12πexp-y22dy(13)

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    Pse=P0Pe0+P1Pe1(14)

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    Ppe=1-(1-Pse)NLaveM(15)

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    Pse,BPWM=12QkgPt,BPWMN0B+12Q(1-k)gPt,BPWMN0B(16)

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    Pse,OOK=12QkgPt,OOKN0B+12Q(1-k)gPt,OOKN0B(17)

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    Pse,PPM=2M-12MQkgPt,PPMN0B+12MQ(1-k)gPt,PPMN0B(18)

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    Pse,DPIM=2M+12M+3QkgPt,DPIMN0B+22M+3Q(1-k)gPt,DPIMN0B(19)

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    Ppe,BPWM=1-1-12QkgPt,BPWMN0B-12Q(1-k)gPt,BPWMN0BN·2M-1MPpe,OOK=1-1-12QkgPt,OOKN0B-12Q(1-k)gPt,OOKN0BNPpe,PPM=1-1-2M-12MQkgPt,PPMN0B-12MQ(1-k)gPt,PPMN0BN·2MMPpe,DPIM=1-1-2M+12M+3QkgPt,DPIMN0B-22M+3Q(1-k)gPt,DPIMN0BN·2M+32M(20)

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    Guifa WANG, Mengyue GUO, Jiamei GU, Min TANG, Zhengjun WEI, Jindong WANG, Shentao WANG. Low Power Consumption Visible Light Communication Technology Based on Bilevel Pulse Width Modulation[J]. Acta Photonica Sinica, 2021, 50(5): 139
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