Methodology for evaluating linear and non-linear effects in a radio over fiber system

Metodología para evaluar los efectos lineales y no lineales en un sistema de radio sobre fibra óptica

Karla Cecilia Puerto López1*, Rudy Paolo Báez Parada2 , Ángel David Torres Palencia3 , Dinael Guevara Ibarra4 .
Abstract

This article shows the methodology used to evaluate the linear and non-linear effects present in a radio over fiber system (RoF) by employing the multiplexing technique used for dense wave division, the Dense Wavelength Division Multiplexing (DWDM) technique. It is completed with a dissemination of 50 GHz, in accordance to the standards of the International Telecommunication Union (ITU), through a channel speed of 10 Gbps, at an input power in the optical channel of 30mW, for optical fiber stretches of 40km, 60km and 80km. It presents the modeling of the RoF system graphically through a block diagram by means Matlab, a computational tool, whereby each of the stages of the RoF system are implemented using the libraries offered by the ‘simulink’ toolbox of Matlab. As a result, it is obtained that the methodology proposed for the evaluation of the RoF system using the DWDM technique allows for the analysis of linear and non-linear effects; where it is observed that the effects that degrade the signal are proportional to the established distances of the optical fiber and that the optical input power used is optimal for the optical fiber to behave as a non-linear medium.

Keywords:Fiber optic, Linear effects, Non-linear effects, System, Radio.

Resumen

En este artículo, se muestra la metodología para evaluar los efectos lineales y no lineales presentes en un sistema de radio sobre fibra óptica (Radio over Fibre, RoF) empleando la técnica multiplexacion por división de onda densa (Dense Wavelenght Division Multiplexing, DWDM) con esparcimientos de 50GHz, según las normas de la Unión Internacional de Telecomunicaciones (International Telecommunication Union, ITU) con una velocidad de canal de 10 Gbps, a una potencia de entrada en el canal óptico de 30mW, para tramos de fibra óptica de 40km, 60km y 80km. Se presenta el modelado del sistema de RoF representado en forma gráfica a través de diagrama de bloques por medio de la herramienta computacional Matlab, donde se implementan cada una de las etapas del sistema de RoF usando las librerías ofrecidas por el Toolbox de simulink de Matlab. Como resultado se obtiene que la metodología propuesta para la evaluación del sistema RoF empleando la técnica DWDM permite analizar los efectos lineales y no lineales; donde se observa que los efectos que degradan la señal son proporcionales a las distancias de la fibra óptica establecidas y que la potencia óptica de entrada empleada es óptima para que la fibra óptica se comporte como medio no lineal.

Palabras clave:Fibra óptica, Efectos lineales, Efectos no lineales, Sistema, Radio.

1. Introduction

Currently the telecommunications companies are undergoing modernization, because in recent years it has become necessary to implement telecommunications systems that can transport a large amount of information and at the same time offer mobility and flexibility at any time to end users of the access network. On the other hand, it has been reported in the scientific literature as a viable option to satisfy the premises described above, generating hybrid patterns that allow the design and implementation of a single telecommunications infrastructure where both optical communications systems and wireless systems converge [1].
Prototypes have been developed internationally, specifically at Dalian University of Technology, in China, where they implement a RoF system with WDM [2], additionally there are studies of these systems with millimeter wave signals in the V and W bands [3]. At a national level, the Pontificia Bolivariana University analyzes the impact on the laser line width requirements due to the linear and non-linear effects introduced by the optical fiber in a WDM-PON transmission system with DPSK modulation format [4]. Locally, at the Francisco de Paula Santander University, a RoF system was modeled under the effects of linear errors using a computational tool [5]. Under these antecedents it can be evidenced that the RoF system under study is with the global, national and local trends.
The integration of optical fiber and wireless networks, such as Radio over Fiber (RoF) systems characterized by combining radio frequency devices with fiber optic links, allowing radio signals from the wireless network to be transported to a remote radiation point by means of optical fiber [6], with an attenuation of 0.25 dB/Km at 1550 nm and providing a large bandwidth of 155 Mb/s for the transmission of information [7].
However, the implementation of optical fiber as a means of data transmission generates undesired errors causing the deformation of the signal carrying information transmitted by the optical channel. These errors can be of linear character such as attenuation and dispersion or non-linear character errors, which are due to the use of semiconductor optical amplifiers or the existing optical powers of the order of +10 dBm present in the fiber input [8], causing the appearance of non-linear effects characteristic of the optical fiber, such as Self- Phase Modulation (SPM), Cross-Phase Modulation (XPM), Four-Wave Mixing (FWM), Scattering Stimulated Brillouin (SBS), and Scattering Stimulated Ramman (SRS).
A system with greater information capacity requires more channels and high bandwidth to provide the services demanded by users, hence the emergence of transmission techniques such as Dense Wavelength Division Multiplexing (DWDM) which is governed under the rules of the International Telecommunication Union (ITU) [9].
This article presents the methodology to perform the modeling and simulation of a RoF system based on the DWDM technique using the Matlab computational tool under the Simulink toolbox. The representative data for the system are: 40km, 60km and 80km fiber optic section, using the eye diagram and constellation diagram as an evaluation technique.
The exposed methodology allows to analyze in a graphic way each stage of the RoF system with DWDM from the Transmitter, Channel and Receiver; where it can be evidenced that a power greater than 10mW generates a widening of the pulses produced by the phenomena of non-linear order.
Below is a description of the methodology used to evaluate the RoF system under these effects using the DWDM technique.

Rof communication system
Radio over optical fiber systems are mixed systems, characterized by taking advantage of optical fiber to transport radio signals directly to the base station [10]. Figure 1 illustrates the scheme and operation of a RoF system consisting of a Control Station, Base Station and a Mobile Station.
• Optical Transmitter: Its main function is to generate the optical millimetre waves, which are responsible for the radio frequency carrier signal to the base station. [10].
• Fibre channel: This is responsible for transporting the radio frequency (RF) signals directly to a remote radiation point according to Figure 1, to the base station. [10].
• Base station: Its main function is opto-electrical conversion. RF signals are sent using high-power amplifiers [10]. (fig 1)


The representation of the RoF system methodology in the computational tool is represented graphically through blocks as you can see in figure 2; it consists of the transmitter block, optical channel and receiver block.

Transmitter Block
This block generates the signal that is sent to the optical channel, where they combine and adapt to the optical channel radio frequency (RF) signals, these signals have a spectrum ranging from 3-300GHz. To adapt the frequencies, ITU standard G.941.1 was used, where the frequencies for the DWDM technique are assigned and is governed by equation 1 [9]. (eq. 1)


linear and non-linear phenomena that degrade the optical signal are presented.
Linear phenomena
At powers less than 10 dBm at the fibre input, linear phenomena arise and are presented below:

Attenuation: Is the loss power of a signal sent through a transmission medium, which can be understood as the loss of power of the light wave when passing through a hard transmission medium [11]. (fig 2)




Where represents the responsiveness, h the plank constate e is the classical electron radius and f represents the central frequency with which the signal is transmitted.

Materials and methods

MatLab is a computational tool that allows you to work with the simulink toolbox, which offers a large library for design, analysis and signal processing. The simulink toolbox is used for the design, analysis and evaluation of the methodology proposed for the RoF system under linear and non-linear effects using the DWDM technique; where the methodology is represented in blocks as shown in figure 2 and then the operation of each block is broken down using the libraries offered by the simulink toolbox [6], [13].

Transmitter block:
The design of this block consists of the signal generation, the optical source and the Mach-Zehnder modulator as shown in Figure 3.
The signal generation block has the function of modulating the RF signal to be taken to electrooptical conversion, using the technique of doublesideband modulation. The optical source block is responsible for generating the optical signal with a frequency stipulated by standard G. 694.1 to be sent to the optical channel, by means of an optical source and thus transmit signals in the third operating window of the optical fiber. The Mach Zehnder modulator block is in charge of converting the RF signal at high frequency to an optical signal and then multiplexing the established optical signals to send them later to the optical channel. (fig 3)


Figure 4 shows the internal components of the signal generation blocks, optical source and Mach Zehnder Modulator implemented in Matlab›s Simulink Toolbox ©.
The methodology used for the implementation of the transmitter block diagram starts with the High Frequency Signal Generation where five signals were generated with EHF carriers and subcarriers modulated using the double sideband method. Table I shows the values of the information carrier and subcarrier signals established for the generation of the analog signal. (fig 4)



For the double sideband modulation the same technique is used for the five generated signals, the signal number 3 is taken as reference and its mathematical equation is governed by equation 7: (7) (eq 7 y 8 )


To perform the process of multiplexing by dense wave division, the G.694.1 [9] standard is used, which for 50GHz spacing defines the allowed channel frequencies (in THz) according to equation (1). Table II shows the frequency values in THz for the five different signals implemented in the optical source, taken from standard G.694.1. (tab 2)


A center frequency of 193.55 THz is used which is the center frequency of the multiplexed signal in the optical channel, this frequency is optimal to operate in a standard single mode fiber which is regulated in standard G.652 of the International Telecommunication Union [14].
Once the millimetre-wave modulated signal has been obtained, the electro-optical conversion is carried out by means of the external Mach Zehnder modulator. The methodology used proceeds to the analysis of the signal treatment, where the general expression of the optical signal obtained at the output of the Mach Zhender modulator must be determined, for which equation 9 of the electric field of the signal at the input [15] is used. (eq 9 y 10)


Subsequently the signals are multiplexed with the optical carriers with a stipulated central frequency of 193.55 GHz, which allows working in the third operating window (1550nm) of the monomode optical fiber standardized by ITU standard G.652.

Optical channel
Figure 5 illustrates the optical channel, which is responsible for signal to the receiver block. For the implementation of the optical are designed: Nonlinear Phase Offset, Nonlinear Order Parameter (fig 5)


For this stage, a standard single-mode optical fi bre governed by standard G.652 is used, presenting the linear and non-linear order parameters used in the design of the channel, as shown in Table III. (tab 3)


The effects of linear and nonlinear origin present in the optical fiber are mathematically modeled through Schrödinger’s nonlinear equation as observed in equation 11.


Optical receiver:
This stage is in charge of receiving the signal after propagating through the optical channel. In the methodology used for the design of the Optical Receiver block, a Photodetector, Filter Bank and a Demultiplexer are used, as shown in fi gure 6. For the implementation of the photodetector in the computational tool, the parameters shown in Table IV are used. (tab 4)


In order to eliminate possible distortions produced by non-linear errors, a bank of fi lters is used, presented in the Simulink toolbox called Filter Design & Analysis Tools. Table V shows the characteristics of the fi lters used to optimise the system. (tab 5)


Figure 7 shows the components that are part of the Receiver block diagram.The proposed methodology (fig 7)


allows to implement step by step the RoF system under the effects of linear and non-linear errors using the DWDM technique in the computational tool and thus evaluate the behavior of the signal under these dispersive effects.
System evaluation
For the evaluation of the RoF system, the technique eye diagram and constellation diagram was used. Figure 8 shows the block diagram implemented in the Simulink toolbox for the eye diagram technique, which consists of an analog/digital converter block and the PCM Modulator block, whose function is to perform the process of converting serial to parallel bits in M (M-aria) samples.
Figure 9 illustrates the block diagram for the constellation diagram evaluation technique, which consists of an analog/digital converter block, PCM Modulator block, and a Phase Shift Modulation block. This block is in charge of performing the signal offset in samples that depend on the M-aria parameter through the M-PSK (phase shift modulator). (fig 5)




The following are the results obtained in the RoF system under the dispersive effects using the proposed methodology.

Results and discussion

With the methodology proposed through the design and implementation of block diagrams for the RoF system through a computational tool, the performance of the proposed methodology is evaluated by performing simulations for different lengths of fiber at 40km, 60km and 80km respectively.
The objective is to track the signals at the input of the transmitter block and the behavior of these signals in the optical channel under linear and non-linear effects and how it behaves in the receiver block.
Five optical signals generated by the optical source are established as shown in Table II, the same number of signals are generated in parallel with the radio frequency carriers established in Table I, where the electro-optical conversion is performed through the Mach Zender modulator and multiplexed with the optical signals established before entering the transmitter channel. This block is in charge of generating enough optical power to make the optical channel behave as a non-linear medium.
Figure 10 illustrates the power level at the fiber input using Spectrum Analyzer from the Simulink toolbox, which evidences a power level of 14.97dBm (30mW) at a frequency of 193.55 THz. (fig 10 , 12 ,13, 14)



The receiver block shows the degradation of the signal produced by the attenuation of the optical fi ber, for the fi ber lengths of 40km, 60km and 80km which is degraded in an attenuation factor of 0.22 dB/km compared to Figure 11.
It is evident that the methodology designed for the RoF communication system is viable since it allows to evaluate the behavior of the signal through the fi ber. The evaluation of the signal transmitted by the RoF communication system is carried out by means of established blocks such as the eye diagram and constellation diagram, where the distance of 80km is established as a reference for the evaluation of the signal behavior since it is the most extensive stretch of the RoF system.
Figure 12 illustrates the result of the block diagram implemented in Matlab Simulink © as shown in Figure 8, of the signal evaluation technique as the eye diagram for a distance of 80km, the conversion of samples of fi xed binary numbers is performed through the PCM modulator, where this number of samples depends on the parameter M-aria (M) which is assigned a dimensionless value of 8. It is evident that the signal has no noise or distortion, this shows that the signal is transmitted is optimal at a distance of 80Km. (fig 12)


Figure 13 illustrates the constellation diagram, which is the result of the block diagram implemented in Matlab simulink as shown in Figure 9, where the phases produced by the M-PSK modulator are evidenced, where M establishes the number of outputs that in this case is assigned a dimensionless value of 8 and correspond to the same phases of outputs of the figure in question. There is a phase shift of the signal of ± 22.5° during the transmission, each phasor presents a condition called tritibit which indicates that there are three bits for each signal evidenced by the yellow dots. It is observed that the signal does not present any noise or distortion. (fig 13)


The following are the conclusions obtained from the proposed methodology for evaluating the RoF system under the effect of linear and non-linear errors.

Conclusions

The Simulink Toolbox is a versatile tool that allows you to make designs based on models and represent them graphically, the RoF system based and designed on a mathematical model could be implemented graphically in the Simulink Toolbox using block diagrams; where the behavior of signals through the optical fiber was evaluated under the effects of linear and non-linear errors using the DWDM technique; where it is evident that the RoF system is optimal at distances of 80km which is the most extensive fiber optic stretch that was assigned for the development of the RoF system model.
The methodology proposed for the evaluation of the RoF system using the DWDM technique allows the analysis of linear and non-linear effects; where it is observed that the effects that degrade the signal are proportional to the distances of the established optical fiber and that the input optical power used is optimal for the optical fiber to behave as a non-linear medium.
The representation of the RoF system through blocks in the computational tool allows to evaluate the behavior of the signal as it is observed in the figures 12, 13 and 14 where there is an ensachamiento of the pulses to the exit of the fiber this is produced by the chirp generated by the nonlinear phenomena XPM and SPM therefore it is evidenced that the power used of 30mW generates that the optical fiber behaves like nonlinear means.
The implementation of the receiver block and the sub-blocks of the eye diagram and the constellation diagram for the evaluation of the system show that the optical power at the input of the 30mW fiber is optimal for the operation of a digital format modulator such as the M-PSK, since it illustrates that the signal does not present distortion by the noise generated by the FWM phenomenon at the established wavelength (1550nm).


References

[1] C. Hernández, G. Enrique, S. Alfaro y G. Paola, “Software de simulación de diferentes tipos de modulación de señales de radiofrecuencia sobre fibra óptica”, Umbral Científico, nº 9, pp. 76-84, 2006.
[2] A. Liu, H. Yin, B. Wu. High-efficient full-duplex WDM-RoF system with sub- central station. Optics Communications. 2018. 414, 72-76. https://doi.org/10.1016/j.optcom.2017.12.068
[3] T. Yang, M. Gao, J. Qian, Y. Zou, L. Xiang, G. Shen. A novel radio-over-fiber system with dual millimeter-wavesignals generated simultaneously. School of Electronics and Information Engineering, Soochow University. 2016. http://dx.doi.org/10.1016/j. ijleo.2016.04.068
[4] J. Álvarez, F. Amaya. Impacto de los efectos lineales y no lineales en el requerimiento del ancho de línea del transmisor en sistemas WDM-DPSK. Rev. UIS Ingenierías, 2015, vol. 14, no 2, p.p. 35-45.
[5] A. Torres, K. C. Puerto, D. Guevara, “Efectos lineales presentes en un sistema de radio sobre fibra óptica empleando multiplexación por división en longitud de onda”, ETCM 2016, Guayaquil , Ecuador, 2016.
[6] N. Masabanda, N. Marmol, “Análisis y Simulación de un Enlace de Radio sobre Fibra Óptica (ROF) a 60 GHz”. Disponible en: http://dspace.ups.edu.ec/ bitstream/123456789/5356/1/UPS-ST001033. pdf. [Último acceso: 07 03 2018].
[7] F. Ramos. “Estudio de efectos no lineales en dispositivos fotónicos y su aplicación en sistemas de radio sobre fibra”. Tesis Doctoral, Universidad Politécnica de Valencia, Abril 6 del 2009.
[8] J. Pérez. “Coexistencia e Integración de Comunicaciones Inalámbricas en Sistemas de Transmisión Ópticos”. Universidad Politécnica de Valencia, Departamento de Comunicaciones. Julio del 2009, pp 1- 193.
[9] Unión Internacional de Telecomunicaciones [online]. Disponible en: https://www.itu.int/ itu-t/recommendations/rec.aspx?rec=10868
[10] Francisco R. Pascual, “Estudio de los Efectos no lineales en dispositivos Fotonicos y su aplicación en sistemas de radio sobre fibra óptica”.
[11] M. L. Calvo “Dispersion Cromática” disponible.http://webs.ucm.es/info/giboucm/ Download/chromatic_dispersion.pdf
[12] F. Gómez, L. A. Garcia, K. C. Puerto, D. Guevara “Modelado De Los Fenómenos No Lineales Generados Por El Efecto ElectroÓptico Kerr En Una Transmisión Por Fibra Óptica”, Rev. Colombiana de Tecnologías de Avanzada, vol. 2, no. 28, pp. 82-87, 2016
[13] Mathworks.com [online]. Disponible en: https://la.mathworks.com/products/simulink. html
[14] Unión Internacional de Telecomunicaciones norma G.652 [online]. Disponible en: https:// www.itu.int/rec/T-REC-G.652/es
[15] F. Marangione. Modelo Simulink para redes de comunicaciones ópticas multiservicio. 2007. Valencia, España.
[16] A. Torres, K. C. Puerto, D. Guevara, “Efectos lineales presentes en un sistema de radio sobre fibra óptica empleando multiplexación por división en longitud de onda”, ETCM 2016, Guayaquil , Ecuador, 2016.
[17] G. Campuzano “Telecomnicaciones Radio Sobre Fibra” disponible [En Linea]. http://www. mty.itesm.mx/die/ddre/transferencia/67/67- III.03.html. [Último acceso: 7 Junio 2017].
[18] G. P. Agrawal, “Fiber-Optic Communication Systems”. 4 a ed. New York, USA: John Wiley & Sons. 2002.
[19] K. C. Puerto, B. Medina, L.L. Camargo “Efecto De La Dispersión Cromática En Un Sistema Híbrido”, Rev. Colombiana de Tecnologías de Avanzada, vol. 2, no. 24, pp. 51-58, 2014.
[20] L. A. Garcia, K. C. Puerto, D. Guevara, “Efectos de la Modulación de Fase Cruzada en comunicaciones por fibra óptica”, VII BETCON, 2015, La Paz, Bolivia, 2015.
[21] A. Stöhr, A. Akrout, R. Buß, B. Charbonnier, F. van Dijk, A. Enard, S. Fedderwitz, D. Jäger, M. Huchard, F. Lecoche, J. Marti, R. Sambaraju, A. Steffan, A. Umbach, M. Weiß. 60 GHz radio-over-fiber technologies for broadband wireless services. Optical Society of America, Journal Of Optical Networking. May 2009, Vol. 8, No. 5 pp 471 – 487.


1* Magíster en Ingeniería de Telecomunicaciones, Orcid: 0000-0003-3749-676X, Universidad Francisco de Paula Santander, Cúcuta, Colombia, karlaceciliapl@ufps.edu.co
2 Ingeniero Electrónico, Orcid: 0000-0002-9018-8486, Universidad Francisco de Paula Santander, Cúcuta, Colombia, rudypaolobp@ufps.edu.co
3 Ingeniero Electrónico, Orcid: 0000-0003-4835-5188, Instituto Nacional de Astronomía Óptica y Electrónica., San Andrés Cholula, México, angeltopa@inaoep.mx
4 Doctor en Ingeniería, Orcid: 0000-0003-3007-8354, Universidad Francisco de Paula Santander, Cúcuta, Colombia, jdinaelgi@ufps.edu.co


Received on January 29, 2018 - Approved on June 12, 2018.
How to cite :K.C. Puerto-López, R.P. Báez-Parada, A.D. Torres-Palencia and D. Guevara-Ibarra, “Methodology for evaluating linear and non-linear effects in a radio over fiber system”, Respuestas, vol. 23, no. 2, pp. 75-88, 2018

Received on January 23, 2018 - Approved on June 06, 2018.