electronics
Article Optical Transmission of an Analog TV-Signal Coded at 2.24 GHz and Its Distribution by Using a Radiating Cable
Ana Gabriela Correa-Mena 1,2 , Jorge Alberto Seseña-Osorio 1, Melissa Eugenia Diago-Mosquera 3, Alejandro Aragón-Zavala 3 and Ignacio Enrique Zaldívar-Huerta 1,* 1 Departamento de Electrónica, Instituto Nacional de Astrofísica, Óptica y Electrónica, Calle Luis Enrique Erro No.1, Tonantzintla, Puebla 72840, Mexico; [email protected] (A.G.C.-M.); [email protected] (J.A.S.-O.) 2 Departamento de Ciencias de la Computación y Electrónica, Universidad Técnica Particular de Loja, San Cayetano Alto, Loja 1101608, Ecuador 3 Escuela de Ingeniería y Ciencias, Tecnológico de Monterrey, Av. Epigmenio González 500, Fracc. San Pablo Querétaro 76130, Mexico; [email protected] (M.E.D.-M.); [email protected] (A.A.-Z.) * Correspondence: [email protected]
Received: 7 May 2020; Accepted: 25 May 2020; Published: 1 June 2020
Abstract: In this work, an alternative technology to extend wireless coverage beyond the conventional methods of providing radio propagation coverage is presented. The use of a radiating cable is proposed for difficult-to-reach areas. In this regard, an indoor radiating cable is successfully employed for the distribution of an analog electric signal in a fiber-radio scheme using a microwave photonic filter. A filtered microwave band-pass window located at 2.24 GHz is used as an electrical carrier to transmit an analog TV-signal of 67.25 MHz over an optical link of 25.28 km. Measurements are carried out in an indoor environment. Experimental results demonstrate that the recovered signal is of good quality in each measurement location, exhibiting on average a signal-to-noise-ratio (SNR) of around 31.60 dB.
Keywords: indoor propagation; microwave photonic filter; microwave signal; radiating cable
1. Introduction The widespread use of mobile communications with broadband applications has increased in recent years. This trend has led to an increase in the demand for the delivery of data and video services to a large number of users in optical and wireless access services, and a greater concentration of mobile devices inside buildings, e.g., university campus, shopping centers, airports, and underground environments. Considering the challenges of this explosive growth, wireless optical communications (WOC) are a good option to provide large bandwidth for users under these scenarios [1]. WOC offers a bundle of advantages, e.g., the electromagnetic spectrum is not licensed in the optical band, thus spectrum licensing fees are avoided and system cost can be reduced. Optical radiation in the infrared or visible range is easily contained by opaque boundaries. As a result, interference between adjacent devices can be minimized easily and economically. Although this contributes to the security of wireless optical links and reduces interference, it also impacts rather stringently on the mobility of such devices [2]. Wireless optical links transmit information by using an optoelectronic light modulator and allow its distribution through fiber optics to users located in indoor environments. In order to provide optimal coverage levels inside buildings, usually, the final distribution in a WOC is implemented through omnidirectional antennas placed at strategic locations. The deployment of these antennas, mainly to address hot-spot areas, may not be possible in outage zones, due to the impossibility of their
Electronics 2020, 9, 917; doi:10.3390/electronics9060917 www.mdpi.com/journal/electronics Electronics 2020, 9, 917 2 of 9
ElectronicsElectronics 2020 2020, ,9 9, ,x x FOR FOR PEER PEER REVIEW REVIEW 22 of of 9 9 installation in specific regions inside venues, their radiation pattern characteristics, and the maximum transmitradiationradiation power pattern pattern limitations. characteristics, characteristics, Therefore, and and the radiatingthe maximum maximum cables transmit transmit have been power power demonstrated limitations. limitations. toTherefore, Therefore, be a viable radiating radiating option tocablescables overcome havehave suchbeenbeen constraints, demonstrateddemonstrated since toto their bebe aa coverage viableviable optionoption footprint toto overcome isovercome uniform suchsuch and canconstraints,constraints, increase since thesince signal theirtheir strengthcoveragecoverage in footprint footprint indoor environments is is uniform uniform and and [3 –can can6]. increase increase the the signal signal strength strength in in indoor indoor environments environments [3–6]. [3–6]. 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BecauseBecauseBecause of ofof this thisthis leakage leakageleakage of ofof signal, signal,signal, line lineline amplifiers amplifiersamplifiers areareare required requiredrequired to toto be bebe inserted insertedinserted at atat regular regularregular intervals, intervals,intervals, typicallytypicallytypically everyevery every 350 350 350 meters meters meters to to to 500 500 500 meters, meters, meters, to to enhanceto enhance enhance the the the signal signal signal back back back up up toup acceptable to to acceptable acceptable levels levels levels [7]. On[7]. [7]. theOn On otherthethe other other hand, hand, hand, an inherentan an inherent inherent feature feature feature of Microwaveof of Microwave Microwave Photonic Ph Photonicotonic Filters Filters Filters (MPFs) (MPFs) (MPFs) is is is that that that microwave microwave microwave signalssignals signals areareare directlydirectly directly processed processed in inin the the optical optical domain, domain, domain, exploiting exploiting exploiting advantages advantages advantages inherent inherent inherent to to photonics tophotonics photonics such such such as as low low as lowloss,loss, loss, high high highbandwidth, bandwidth, bandwidth, immunity immunity immunity to to electromagneti electromagneti to electromagneticcc interference, interference, interference, and and tunability tunability and tunability [8], [8], making making [8], making them them a a themveryvery interesting ainteresting very interesting choice choice compared compared choice compared to to conventional conventional to conventional el electricalectrical electricalfilters. filters. The The filters. factors factors The previously previously factors previously described, described, described,togethertogether with with together the the increasing increasing with the increasing demand demand for demandfor multiple multiple for communications multiple communications communications applications applications applications with with a a great great with amount aamount great amountofof associatedassociated of associated information,information, information, justifyjustify justify thethe introductionintroduction the introduction ofof MPFsMPFs of MPFs intointo into thethe the accessaccess access opticaloptical optical networks networksnetworks [[9].9[9].]. Furthermore,Furthermore,Furthermore, a a comparisona comparisoncomparison between betweenbetween our our proposedour propospropos fiber-radioeded fiber-radiofiber-radio scheme schemescheme with the withwith WOC’s thethe works WOC’sWOC’s reported worksworks inreportedreported the last in in few the the yearslast last few few is presentedyears years is is presented presented in Table1 in .in TheTa Tableble parameters 1. 1. The The parameters parameters considered considered considered are the frequencyare are the the frequency frequency of the electricalofof the the electrical electrical carrier, carrier, carrier, the signal-to-noise-ratio the the signal-to- signal-to-noise-rationoise-ratio of the of recoveredof the the recovered recovered signal signal signal (SNR RX(SNR (SNR), theRXRX),), fiber the the fiber length,fiber length, length, and and theand transmisionthethe transmision transmision and and receptionand reception reception of the of of signalthe the signal signal by using by by using using radiating radiating radiating cable cable cable and antennas,and and antennas, antennas, respectively. respectively. respectively.
TableTableTable 1.1. 1. RelevantRelevant Relevant worksworks works thatthat that considerconsider consider wirelesswireless wireless opticaloptical optical communicationscommunications communications (WOC).(WOC). (WOC).
SNRSNRRXRX FiberFiberFiber Coil CoilCoil Ref.Ref.Ref. CarrierCarrierCarrier (GHz) (GHz) (GHz) SNR (dB) RadiatingRadiatingRadiating Cable Cable Wireless Wireless Wireless Reception Reception (dB)RX(dB) (km)(km) 200720072007 [ 10[10] [10]] 60 60 60 26 26 26 SMF: SMF: 20 2020 2008 [11] 4 - SMF: 4 20082008 [11] [11] 4 4 - - SMF: SMF: 4 4 2015 [12] 2.27; 4.54 38.25; 37.83 SM-SF: 25.24 201620152015 [[12]3 [12]] 2.27;0.9–2.3 2.27; 4.54 4.54 38.25; 38.25;39 37.83 37.83 SM-SF: SM-SF: SM-SF: 25.24 25.2425.24 ≈ 201720162016 [13 [3] [3]] 0.9–2.3 2.40.9–2.3 38.8≈≈ 39 39 SM-SF: SM-SF: SM-SF: 25.24 25.24 30 2018 [14] 60 - SMF: 2.2 201820172017 [ 15[13] [13]] 60 2.4 2.4 38.8 38.8- SM-SF: SM-SF: SMF: 2.2 30 30 This20182018 work [14] [14] 2.24 60 60 36.53 - - SM-SF: SMF: SMF: 2.2 25.282.2 20182018 [15] [15] 60 60 - - SMF: SMF: 2.2 2.2 Considering the main goal of this work is to demonstrate the feasibility of distribution by a ThisThis work work 2.24 2.24 36.53 36.53 SM-SF: SM-SF: 25.28 25.28 radiating cable of an analog TV-signal in a fiber-radio scheme inside a building, a band-pass window at 2.24 GHz generated by a microwave photonic filter is used to code on the analog TV signal of ConsideringConsidering the the mainmain goalgoal ofof this this workwork isis to to demonstratedemonstrate thethe feasibility feasibility ofof distributiondistribution byby aa 67.25 MHz. This TV signal is transmitted over an optical link of 25.28 km for its further distribution by radiatingradiating cable cable of of an an analog analog TV-signal TV-signal in in a a fiber-radio fiber-radio scheme scheme inside inside a a building, building, a a band-pass band-pass window window a radiating cable of 5.50 m length. The novelty of this work resides in the integration of the radiated atat 2.24 2.24 GHz GHz generated generated by by a a microwave microwave photonic photonic filter filter is is used used to to code code on on the the analog analog TV TV signal signal of of cable technique with the fiber scheme to transmit and distribute electrical signals, using optoelectronic 67.2567.25 MHz. MHz. This This TV TV signal signal is is transmitted transmitted over over an an optical optical link link of of 25.28 25.28 km km for for its its further further distribution distribution techniques and its further radio distribution in an indoor environment. Thus, this fiber-radio scheme byby a a radiating radiating cable cable of of 5.50 5.50 m m length. length. The The novelty novelty of of this this work work resides resides in in the the integration integration of of the the radiated radiated could be used as part of a wireless optical communication system. cablecable techniquetechnique withwith thethe fiberfiber schemescheme toto transmittransmit andand distributedistribute electricalelectrical signals,signals, usingusing The paper is organized as follows: Section2 provides the basic theory of the MPF operation optoelectronicoptoelectronic techniquestechniques andand itsits furtherfurther radioradio distdistributionribution inin anan indoorindoor environment.environment. Thus,Thus, thisthis principle. Moreover, the experimental frequency response of the characterized MPF is presented. fiber-radiofiber-radio scheme scheme could could be be used used as as part part of of a a wireless wireless optical optical communication communication system. system. The experimental procedure for the transmission, distribution, and recovery of the analog TV-signal is TheThe paper paper is is organized organized as as follows: follows: Section Section 2 2 pr providesovides the the basic basic theory theory of of the the MPF MPF operation operation described in Section3. Finally, the main conclusions are included in Section4. principle.principle. Moreover, Moreover, the the experimental experimental frequency frequency resp responseonse of of the the characterized characterized MPF MPF is is presented. presented. The The 2.experimentalexperimental Microwave procedure Photonicprocedure Filter for for the the tran transmission,smission, distribution, distribution, and and recove recoveryry of of the the analog analog TV-signal TV-signal is is describeddescribed in in Section Section 3. 3. Finally, Finally, the the main main conclusions conclusions are are included included in in Section Section 4. 4. This section is divided in two subsections. First, the main equations that describe the frequency response2.2. Microwave Microwave of the Photonic Photonic MPF are Filter detailed.Filter In the second subsection, the MPF is characterized to obtain the electrical parameters of the filtered band-pass windows that will be used as electrical carriers. ThisThis section section is is divided divided in in two two subsections. subsections. First, First, the the main main equations equations that that describe describe the the frequency frequency responseresponse of of the the MPF MPF are are detailed. detailed. In In the the second second su subsection,bsection, the the MPF MPF is is characterized characterized to to obtain obtain the the electricalelectrical parameters parameters of of the the filtered filtered band-pass band-pass wi windowsndows that that will will be be used used as as electrical electrical carriers. carriers.
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2.1. Principle of Operation 2.1. Principle of Operation Previously, the authors of [16] reported the use of a basic architecture of MPFs that consist of Previously, the authors of [16] reported the use of a basic architecture of MPFs that consist of four four basic components: an optical source, a modulator, a fiber coil, and a photodetector. The basic components: an optical source, a modulator, a fiber coil, and a photodetector. The frequency frequency response of this MPF is constituted of a series of microwave band-pass windows that response of this MPF is constituted of a series of microwave band-pass windows that depend on the depend on the fiber chromatic dispersion, fiber length, and Fourier transform of the spectral density fiber chromatic dispersion, fiber length, and Fourier transform of the spectral density of the optical of the optical source. In particular, when a Multimode Laser Diode (MLD) is used as an optical source. In particular, when a Multimode Laser Diode (MLD) is used as an optical source, the theoretical source, the theoretical center frequency of the nth filtered band-pass window is computed as [16] center frequency of the nth filtered band-pass window is computed as [16] 1 = 1 (1) fn = n (1) where n is a positive integer (n = 1, 2, …), δλ (nm) is DLtheδλ Free Spectral Range (FSR) between the modes ofwhere the MLD,n is a positiveand L (km) integer and (Dn =(ps/nm·km)1, 2, . . . ), δλ are(nm) the islength the Free and Spectral the chromatic Range (FSR)dispersion between of the the Single modes Mode-Standardof the MLD, and FibreL (km) (SM-SF), and D (psrespectively./nm km) are The the bandwidth length and at the −3dB chromatic of the dispersionnth filtered of band-pass the Single · windowMode-Standard is obtained Fibre as (SM-SF),[16] respectively. The bandwidth at 3dB of the nth filtered band-pass − window is obtained as [16] 4 ln(2) Δ = p (2) Δ 4 ln(2) ∆ fbp = (2) where Δλ (nm) is the spectral width of the optical source.πDL∆λ where ∆λ (nm) is the spectral width of the optical source. 2.2. Experimental MPF Characterization 2.2. Experimental MPF Characterization Figure 1 shows the microwave photonic filter scheme that is characterized. The MPF is composedFigure of1 showsan optical the microwave source MLD, photonic a Polariza filter schemetion Controller that is characterized. (PC), a Mach–Zehnder The MPF is composed Intensity Modulatorof an optical (MZ-IM), source a MLD, Microwave a Polarization Signal Generator Controller (MSG), (PC), aan Mach–Zehnder SM-SF, and a Photo Intensity Detector Modulator (PD). The(MZ-IM), Electrical a Microwave Spectrum Signal Analyzer Generator (ESA) (MSG),is used anto SM-SF,measure and the a frequency Photo Detector response (PD). of The the Electrical system. TheSpectrum MLD is Analyzer driven at (ESA) 25 °C is by used a temperature to measure thecontroller frequency and response operated of with the system.a well-stabilized The MLD injection is driven currentat 25 ◦C of by 20 amA. temperature Under this controller condition, and its op operatedtical characteristics with a well-stabilized are central wavelength injection current λ0 = 1547.2 of 20 nm, mA. ΔλUnder = 7.31 this nm, condition, and δλ = its 1.1 optical nm. characteristics are central wavelength λ0 = 1547.2 nm, ∆λ = 7.31 nm, and δλ = 1.1 nm.
Figure 1. Scheme of the microwave photonic filter.
The light issued of theFigure MLD 1. (Thorlabs, Scheme of LPS-1550-FC) the microwave passesphotonic through filter. the PC. Subsequently, it is injected to the MZ-IM (MXAN-LN-20, insertion loss of 2.7 dB, operating wavelength of 1530 nm to 1580The nm) light where issued it is intensity-modulated of the MLD (Thorlabs, by an LPS-1550- RF signalFC) supplied passes bythrough the MSG the in PC. the Subsequently, frequency range it is of injected0.01 GHz to to the 10 MZ-IM GHz at an(MXAN-LN-20, electrical power insertion of 5 dBm. loss The of 2.7 modulated dB, operating light travels wavelength along 25.28of 1530 km nm of theto 1580SM-SF nm) (α where= 0.2 dB it is/km, intensity-modulated D = 15.81 ps/nm km by @ an 1500 RF signal nm). At supplied the output by the of theMSG fiber, in the the frequency PD (DR-125G-A, range · of30 0.01 kHz GHz to 12.5 to GHz)10 GHz converts at an electrical the light power to its corresponding of 5 dBm. The photo-current. modulated light This travels experiment along 25.28 is carried km ofout the at SM-SF the maximum (α = 0.2 dB/km, PD frequency D = 15.81 of 10ps/nm·km GHz. Finally, @ 1500 the nm). electrical At the signaloutput at of the the PD’s fiber, output the PD is (DR-125G-A,amplified and 30 connected kHz to 12.5 to the GHz) ESA converts (Anritsu, the MG3692, light to frequency its corresponding range 0.01 photo-current. GHz to 20 GHz) This to experiment is carried out at the maximum PD frequency of 10 GHz. Finally, the electrical signal at measure the MPF’s frequency response. This experimental frequency response is formed by four the PD’s output is amplified and connected to the ESA (Anritsu, MG3692, frequency range 0.01 GHz microwave band-pass windows, as shown in the blue curve of Figure2. The center frequency of to 20 GHz) to measure the MPF’s frequency response. This experimental frequency response is each filtered band-pass window is f 1 = 2.24 GHz, f 2 = 4.40 GHz, f 3 = 6.62 GHz, and f 4 = 8.86 GHz. formed by four microwave band-pass windows, as shown in the blue curve of Figure 2. The center On the same graph, the black curve corresponds to the theoretical frequency response obtained by frequency of each filtered band-pass window is f1 = 2.24 GHz, f2 = 4.40 GHz, f3 = 6.62 GHz, and using the VPIphotonics software [17], and it is in good concordance with the experimental response. f4 = 8.86 GHz. On the same graph, the black curve corresponds to the theoretical frequency response obtained by using the VPIphotonics software [17], and it is in good concordance with the
ElectronicsElectronics 2020,2020 9, x, FOR9, 917 PEER REVIEW 4 of 94 of 9 experimental response. Additionally, the increase in attenuation observed in the frequency response plot asAdditionally, frequency the increases increase is in justified attenuation by observedthe influence in the of frequency the envelope response of plotthe assource frequency power increases spectrum, is justified by the influence of the envelope of the source power spectrum, as was demonstrated by the as was demonstrated by the authors of [13]. The interested reader can see this reference for a detailed authors of [13]. The interested reader can see this reference for a detailed explanation. explanation.
FigureFigure 2. Frequency 2. Frequency response response of of the microwave photonic photonic filter. filter.
Table2 summarizes the electrical characteristics of the filtered band-pass windows. Relevant Table 2 summarizes the electrical characteristics of the filtered band-pass windows. Relevant parameters shown are: the center frequency and bandwidth of each band-pass window computed parameters shown are: the center frequency and bandwidth of each band-pass window computed by by using Equations (1) and (2), respectively; the Signal-to-Noise-Ratio (SNR) and the related error using Equations (1) and (2), respectively; the Signal-to-Noise-Ratio (SNR) and the related error percentage between the theoretical and experimental center frequency fn are calculated as percentage between the theoretical and experimental center frequency fn are calculated as