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.
ResumenEn 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 methodsMatLab 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).
[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