基于光子波形发生器产生高效超宽带信号的研究
2016-11-07张大伟
李 征,戴 博,,王 旭,张大伟
(1.上海理工大学 光电学院 上海市现代光学系统重点实验室,上海 200093;2.赫瑞瓦特大学 光电子与量子科学研究所,爱丁堡 EH144AS,英国)
基于光子波形发生器产生高效超宽带信号的研究
李征1,戴博1,2,王旭2,张大伟1
(1.上海理工大学 光电学院 上海市现代光学系统重点实验室,上海200093;2.赫瑞瓦特大学 光电子与量子科学研究所,爱丁堡EH144AS,英国)
利用一个多功能光子波形发生器生成一组5.5 GHz超宽带信号。多功能光子波形发生器由一个单级双驱动马赫曾德尔调制器及一段单模光纤组成,通过调节双驱动马赫曾德尔调制器的输入射频信号及直流偏置,以及单模光纤的色散,可以产生单峰脉冲、双峰脉冲和一个具有高功率谱效率的超宽带信号,产生的超宽带信号完全符合美国联邦通信委员会制定的室内通信辐射限制要求,普通的单峰脉冲和双峰脉冲的光功率谱效率分别可以达到0.1%和0.74%,经过变量特殊设置,可以产生一个高效的超宽带信号,其功率谱效率可以高达24.03%。这种超宽带信号发生器可以用于室内定位、室内通讯等领域。
超宽带; 调制技术; 信号处理; 信号产生; 光载无线通信
Introduction
Ultrawide band (UWB) radio communication is regarded as one of the promising techniques for the next-generation high-data-rate short-range wireless communication systems because of its advantages of low cost,low power consumption,high capacity and multipath robust[1-3].Various schemes of UWB signal generation have been proposed by means of photonic techniques,including electro-optic phase modulation,relaxation oscillations of a semiconductor laser and cross-phase modulation in a semiconductor optical amplifier,to realize UWB-over-fiber technology as well as to reduce the use of expensive high-speed radio frequency (RF) components[4-7].The key challenge of UWB signal generation is to meet the requirement of spectral mask specified by the federal communications commission (FCC)[8].However,some well-known UWB signals,such as monocycle and doublet pulses,have low-frequency components,which may interfere with the global positioning system (GPS) (GPS band at 0.96~1.61 GHz).Thus,the power attenuation is needed for these UWB signals to avoid disturbance to the GPS systems,resulting in low spectral power efficiency.As a result,UWB systems using monocycle and doublet pulses have spectral power efficiency of only 0.12% and 1.38%,respectively[9-10].
Now,we put a novel scheme to generate a group of 5.5 GHz UWB signals.Owing to high coherence,good stability and low cost,dual-drive Mach-Zehnder modulator (DD-MZM),which was driven by two RF signals and controlled by two direct-current (DC) bias in the two arms of a MZM,was used in the many photonic microwave applications,we use our previously proposed photonic versatile waveform generator,which has been theoretically studied and experimentally demonstrated to generate short pulse and trapezoidal,triangular and sawtooth waveforms from a continuous-wave (CW) light at a repetition rate of 10 GHz[11-12],to generate monocycle and doublet pulses,which are widely used in the current UWB systems.To use RF spectrum efficiently,the generation of high-spectral-power-efficiency UWB signals is desired.Thus,we use the generator to generate a spectral-power-efficient UWB signal.
1 Theoretical Model
The setup of photonic versatile waveform generator is shown in Fig.1.The waveform generation is based on single-stage dual-drive Mach-Zehnder modulation and chromatic dispersion.A CW laser is used as a light source,whose center wavelength is tunable.The CW light is injected into a dual-drive Mach-Zehnder modulator (DD-MZM),which is modulated by two sinusoidal RF signals and driven by two DC bias voltages.The RF signals on the two branches are generated by using a RF synthesizer and a 3 dB coupler.The powers of the two RF signals are adjusted by two RF attenuators.The one RF signal is delayed by a RF phase shifter to produce some relative phase shift between the two RF signals.The modulated light is then fed into a span of single-mode fiber (SMF),which is used to induce chromatic dispersion for the formation of waveforms.A following photodetector (PD) is employed to convert the optical signal into electrical signal.In the waveform generator,there are four variables,the amplitudesA1andA2, the phase shiftφof the two RF signals,the difference of two DC bias voltages (VBias1-VBias2) and induced chromatic dispersion,which is determined by the length of the fiberz,affecting the generation of waveform.
In the calculation,both switching voltage and switching bias voltage of the DD-MZM are 4 V.The frequency of the two RF signals is 1 GHz.The center wavelength of CW light is 1550 nm.Only first-order chromatic dispersion is considered.The chromatic dispersion coefficient is 17 ps/(nm·km-1)The bandwidth of PD is 40 GHz.
Fig.1 Setup of photonic versatile waveform generator.
2 Generation of UWB signals
Versatile waveforms can be generated from the generator by controlling the variables.A monocycle pulse is generated whenA1=6 V,A2=4 V,VBias1-VBias2=1 V,the length of SMF is 200 m and the delay between the two RF signals is 45 ps.The generated waveform and the power spectral density with the FCC indoor emission mask are shown in Fig.2.The pulse width is about 150 ps.The power spectral density of the monocycle pulse is not FCC compliant.To avoid the interference with GPS,the signal is attenuated to ensure that its low-frequency component is below the FCC indoor emission mask.The spectral power efficiency is calculated within the frequency band for communications and field disturbance sensing (3.1~10.6 GHz),as follows.
Fig.2 Generation of monocycle pulse
(1)
wherePFCC(f) is the FCC power spectral density mask andY(f) is the power spectral density of the generated signal.
The spectral power efficiency of the generated monocycle pulse is only 0.1%.The utilization of the spectrum is very low.
In the generation of doublet pulse,the amplitudes of the RF signals and the DC bias voltages becomeA1=5 V,A2=5 V,VBias1=4 V andVBias2=0 V.A 175 ps delay is added to one of the RF signals,corresponding to a phase shift of 0.35π.The length of SMF is kept 200 m.The waveform of the doublet pulse is illustrated in Fig.3(a).The doublet pulse is symmetric and has a deep dip in the middle.The power spectral density of the doublet pulse is plotted together with the FCC indoor emission mask in Fig.3(b).The power spectrum of the doublet pulse is centered around 6.5 GHz and has a 10 dB bandwidth of about 6 GHz,which fits well the FCC-specified spectral mask.Besides,there is a notch around the GPS band.However,the power spectral density of the doublet pulse is not fully FCC compliant.The low-frequency components still exist.Therefore,the power of the doublet pulse is attenuated to fit the FCC mask.The resultant spectral power efficiency is 0.74%.
Fig.3 Generation of doublet pulse
To generate a spectral-power-efficient signal,we searching the values of the variables to generate a signal whose spectral power density is below FCC mask and which has the highest spectral power efficiency within the frequency band of 3.1~10.6 GHz.First of all,the spectral power density of the target waveform is calculated,which are the conditions of the waveform generation.Secondly,original values are assigned to the four variables and the roughly searching ranges are given to generate waveforms.Lastly,the properties of the generated waveform are calculated and compared with the target waveform.If they are unmatched,we change the values of the variables one by one for another round of matching.The values of the variables are obtained as follows:A1=6 V,A2=4 V,VBias1=2 V andVBias2=0 V.The delay of one RF signal is 20 ps and the length of the SMF becomes 450 m.Which can generate a larger chromatic dispersion.The shape of the signal is oscillated,as shown in Fig.4(a).The power spectrum is centered at 5.5 GHz and the 10 dB bandwidth is about 7 GHz,as shown in Fig.4(b).A notch appears at the GPS band and the low-frequency components are relatively weak comparing with those within the 3.1~10.6 GHz.The power spectral density is almost FCC compliant.The calculated spectral power efficiency is 24.03%,which is significantly improved.Compared to the monocycle and doublet pulses,the spectral-power-efficient UWB signal efficiently utilizes the RF spectral resource.
Fig.4 Generation of spectral-power-efficient signal
3 Conclusion
We have proposed the generation of monocycle and doublet pulses and a spectral-power-efficient UWB signal using a simple-structured photonic versatile waveform generator.Monocycle and doublet pulses are widely used in the current UWB systems.However,the spectral power efficiencies of the monocycle and doublet pulses are very low.Furthermore,to achieve high spectral power efficiency,we have developed the algorithm to determine the variables for generating spectral-power-efficient UWB signal.Comparing to the monocycle and doublet pulses,the generated spectral-power-efficient UWB signal fits the FCC indoor emission mask well and has the spectral power efficiency of up to 24.03%,which is a desired UWB signal and very suitable for the UWB systems.
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(编辑:张磊)
Study on generation of spectral-power-efficient ultrawide band signal from photonic versatile waveform generator
LI Zheng1,DAI Bo1,2,WANG Xu2,ZHANG Dawei1
(1.Shanghai Key Lab of Modern Optical System,School of Optical-Electrical and Computer Engineering,University of Shanghai for Science and Technology,Shanghai 200093,China;2.Institute of Photonics and Quantum Sciences,Heriot-Watt University,Edinburgh,EH144AS,United Kingdom)
A photonic versatile waveform generator is used to generate a group of 5.5 GHz ultrawide band (UWB) signals.The photonic versatile waveform generator consists of a single-stage dual-drive Mach Zehnder modulator and a span of single-mode optical fiber.By adjusting two input radio-frequency signals and two direct-current bias of the modulator and the chromatic dispersion of the fiber,monocycle pulse,doublet pulse and a specific UWB signal can be generated.The power spectral density of the generated signals fits the Federal Communications Commission indoor emission mask well.The monocycle pulse and doublet pulse have spectral power efficiencies of 0.1% and 0.74%,respectively.For a special setting,the generator can generate a kind of UWB signal of up to 24.03% spectral power efficiency.The UWB signal generator can be used for indoor positioning and indoor communication applications.
ultrawide band (UWB); odulation technique; signal processing; signal generation; radio over fiber
2016-01-14
国家自然科学基金资助项目(61378060);上海市浦江人才计划项目(14PJ1406900)
李征(1989—),男,硕士研究生,主要从事微波光子学、光通信等方面的研究。E-mail:15655917889@163.com
张大伟(1977—),男,教授,主要从事光学薄膜、亚波长光栅等方面的研究。E-mail:dwzhang@usst.edu.cn
1005-5630( 2016) 03-0238-05
TH 29
A
10.3969/j.issn.1005-5630.2016.03.009