MIME-Version: 1.0 Content-Type: multipart/related; boundary="----=_NextPart_01DAECE7.169D2990" Este documento es una página web de un solo archivo, también conocido como archivo de almacenamiento web. Si está viendo este mensaje, su explorador o editor no admite archivos de almacenamiento web. Descargue un explorador que admita este tipo de archivos, como Windows® Internet Explorer®. ------=_NextPart_01DAECE7.169D2990 Content-Location: file:///C:/4E87DED5/02DIEGOTORRES-ExplorandoladispersionpormododepolarizacionenfibraopticaNZDSFunanalisissegunITU-TG.655.htm Content-Transfer-Encoding: quoted-printable Content-Type: text/html; charset="us-ascii" Title

Explorando la dispersión por modo de polarización en f= ibra óptica NZDSF: un análisis según ITU-T G.655=

 

= Exploring polarization mode dispersion in NZDSF Optical Fiber: An analysis according = to ITU-T G.655

1=

Diego Andrés Torres Clavijo 

https://= orcid.org//0009-0007-2050-2234

 

 

Escuela Superior Politécnica de Chimboraz= o/ Facultad de Informática y Electrónica

d= iegoa.torres@espoch.edu.ec   

2=

Oswaldo Geovanny Martínez Guashima                 https://orcid.org//0000-0001-9018-7777

Escuela Superior Politécnica de Chimborazo/ Facultad de Informática= y Electrónica

omartinez@espoch.edu.ec  

 

3

Jaime David Camacho Castillo        &nbs= p;            &= nbsp;          https://orcid.org//0000-0002-9110= -6585

Escuela Superior Politécnica de Chimboraz= o/ Facultad de Informática y Electrónica

= jaimed.camacho@espoch.edu.ec  

4

Joffre Stalin Monar Monar       &nbs= p;                     &nbs= p;          https://orcid.o= rg//0000-0002-6534-183X

Escuela Superior Politécnica de Chimboraz= o/ Sede Orellana

jmonar@e= spoch.edu.ec

&n= bsp;

&n= bsp;

&n= bsp;

&n= bsp;

 

 

Artículo de Investigación Científica y Tecnológica

Enviado: 15/05/2024

Revisado: 14/06/2024

Aceptado: 31/07/2024

Publicado:09/08/2024

DOI:   https://doi.org/10.33262/ap.v6i3.1.515<= /span>  <= span style=3D'mso-spacerun:yes'>        &nbs= p;         

<= span style=3D'font-size:12.0pt;line-height:115%;mso-fareast-font-family:Calibr= i; color:blue;mso-ansi-language:ES-EC'> 

 

 =

Cítese: =

 

 

Torres Clavijo , D. A., Martínez Guashima, O. G., Camacho Castillo, J. D., & Monar Monar, J. S. (2024). Explorando la dispersión por modo de polarización en fibra óptica NZDSF: un análisis según ITU-T G.655. AlfaPub= licaciones, 6(3.1), 34–48. https://doi.org/10.33262/= ap.v6i3.1.515

 

 

 

ALFA PUBLICACIONES, es una revis= ta multidisciplinar, trimestral, que se publicará en soporte electrónico tiene como misión contribuir a la   formación de profesionales competentes con visión humanística y crítica que sean capaces de exp= oner sus resultados investigativos y científicos en la misma medida que= se promueva mediante su intervención cambios positivos en la sociedad. https://alfapublicaciones.com<= u>  

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<= span style=3D'font-size:8.0pt;line-height:115%;mso-fareast-font-family:Calibri; mso-ansi-language:ES-EC'>Esta revista está protegida bajo una lice= ncia Creative Commons Attribution Non Commercial No Derivatives 4.0 Internatio= nal. Copia de la licencia: http://creativecommons.org/license= s/by-nc-nd/4.0/

 

Palabras claves:

PMD, simuladores, pre-compensadores, post-compensadores, fibra óptica.

 

Resumen

Introducción: Este artículo aborda la crucial problemática de la dispersión por modo de polarizació= ;n (PMD) en sistemas de comunicación óptica, evaluando la efectividad de pre-compensadores y post-compensadores en su mitigaci&oacu= te;n. Objetivo: Analizar las características principales del fenómeno de dispersión por modo de polarización (PMD= ) en fibras ópticas NZDSF. Metodología: Se realizaron simulaciones en diversos escenarios, considerando variables como longitud de onda, distancia de transmisión y veloci= dad de transmisión. Resultados: Los resultados destacan la complejidad del desafío y la variabilidad en la eficacia de los compensadores, con hallazgos prometedores en la mejora de la calidad y confiabilidad de la transmisión óptica, especialmente con l= os posts compensadores. Sin embargo, se señala la necesidad de ajustes adicionales para optimizar su desempeño en entornos específicos. Conclusió= n: Este estudio subraya la importancia de abordar de manera cuidadosa y adaptable los desafío= s de dispersión en sistemas de fibra óptica para garantizar un rendimiento óptimo en diversas condiciones operativas. Área de estudio general: Ingeniería de Telecomunicaciones. Área de estudio específica: Fibras ópticas. Tipo de estudio: Original investigati= vo.

 

 

Keywords: PMD, simulators, pre compensators, post compensators, optical fiber.<= /p>

 

Abs= tract<= o:p>

Introduction: This article addresses the crucial problem of polarization mode scattering (PMD) in optical communication systems, evaluating the effectiveness of compensators and post-compensators in the= ir mitigation. Objective: To analyze the main characteristics of the phenomenon of scattering by polarization mode (PMD) in optical fibers NZD= SF. Methodology: Simulations were performed in various scenarios, considering variables su= ch as wavelength, transmission distance and transmission speed. Results:<= /b> The results highlight the complexity of the challenge and the variability= in the efficiency of the compensators, with promising findings in the improvement of quality and reliability of optical transmission, especially with post compensators. However, it points to the need for additional adjustments to optimize its performance in specific environments. Conc= lusion: This study underlines the importance of carefully and flexibly addressing= the challenges of dispersion in optical fiber systems to ensure optimum performance in various operating conditions. General area of study: Telecommunications Engineering. Specific area of study: Optical fibers. Type of study: Original research

 

 

&n= bsp;

Introdu= cción

La dispersión por modo de polarización (PMD) es un fenóme= no inherente en las fibras ópticas que puede afectar significativamente= la calidad de la transmisión de datos en sistemas de comunicació= n de alta velocidad (Alustiza et al., 2019). En este contexto, las fibras ópticas de índice gradual con dispersión no nula de la velocidad de grupo (NZDSF) son ampliamente utilizadas debido a su capacidad para minimizar la dispersión cromática, pero aún prese= ntan desafíos relacionados con la PMD.

El estándar ITU-T G.655 proporciona especificaciones para las fibras ópticas NZDSF, incluyendo criterios para la PMD. Este estándar establece parámetros que influyen en la dispersión, como la velocidad de transmisión, la longitud de la fibra y el coeficiente de PMD, con el objetivo de garantizar una transmisión confiable en ento= rnos de alta velocidad y larga distancia (Cadena & Jiménez, 2019).

El presente análisis se centra en explorar las características principales de la dispersión por modo de polarización en fibr= as ópticas NZDSF de acuerdo con el estándar ITU-T G.655, utiliza= ndo simulaciones para evaluar los efectos de diferentes parámetros en la transmisión de datos. Se examinarán los niveles de dispersión y atenuación de los pulsos de luz, así como= el impacto del retardo diferencial de grupo (DGD) en la calidad de la transmisión.

A través de este estudio, se busca comprender cómo la PMD afect= a la integridad de la señal óptica en las fibras ópticas NZ= DSF y cómo pueden mitigarse estos efectos para garantizar una transmisión eficiente y confiable en sistemas de comunicación= de próxima generación.

Fibra óptica

En el contexto de esta investigación, la fibra óptica desempeña un papel crucial en el estudio de la dispersión por modo de polarización (PMD). La PMD es un fenómeno que ocurre = en las fibras ópticas debido a las variaciones en la velocidad de propagación de los diferentes modos de polarización de la luz. Estas variaciones pueden provocar distorsiones en la señal luminosa,= lo que afecta la integridad de la transmisión de datos (Chepkoiwo et al= ., 2020).

La fibra óptica utilizada en esta investigación es la de índice gradual con dispersión no nula de la velocidad de grup= o (NZDSF), que se caracteriza por tener una distribución gradual del índ= ice de refracción a lo largo de su núcleo. Esta estructura permite minimizar la dispersión cromática, lo que la hace adecuada pa= ra aplicaciones de alta velocidad y larga distancia. Sin embargo, la PMD sigue siendo un desafío en estas fibras y es crucial comprender su impacto para optimizar el rendimiento de los sistemas de comunicación (Cot&i= acute;, 2022).

La relevancia de la fibra óptica en esta investigación radica en= su papel como medio de transmisión para estudiar los efectos de la PMD.= Al comprender cómo la luz se propaga a través de la fibra y cómo interactúa con sus características físicas, podemos identificar estrategias para mitigar los efectos adversos de la PMD= y mejorar la calidad de la transmisión de datos en las redes ópticas (Landivar, 2021).

La fibra óptica también es relevante en el contexto de la normat= iva internacional establecida por el estándar ITU-T G.655. Este estándar define las especificaciones para las fibras ópticas NZDSF, incluidos los parámetros relacionados con la PMD. Al seguir e= stas especificaciones, los fabricantes garantizan que las fibras ópticas cumplan con ciertos estándares de calidad y rendimiento, lo que es fundamental para el desarrollo y despliegue de sistemas de comunicaci&oacut= e;n confiables (Sánchez et al., 2023).

Fibras Ópticas de Dispersión Desplazada No Nula (NZDSF)

Estas fibras se caracterizan por tener una dispersión de la velocidad de g= rupo que se desplaza hacia valores no nulos en la longitud de onda de operaci&oa= cute;n, lo que las hace ideales para aplicaciones de comunicaciones ópticas = de alta velocidad y larga distancia.

La principal ventaja de las fibras ópticas NZDSF es su capacidad para minimizar la dispersión cromática en la banda de longitud de = onda utilizada para la transmisión de datos, lo que permite una transmisión más eficiente y con menor distorsión de la señal. Esto se logra mediante un diseño especial de la fibra = que ajusta la distribución de la dispersión de la velocidad de gr= upo para que coincida con la longitud de onda de operación (Peñar= anda & Rodríguez, 2019).

Además de su capacidad para mitigar la dispersión cromática, las fib= ras ópticas NZDSF también pueden reducir otros efectos no lineale= s no deseados, como la dispersión intramodal y la dispersión por m= odulación de fase, lo que contribuye a una transmisión más confiable de datos a largas distancias y altas velocidades.

Las fibras ópticas NZDSF se utilizan ampliamente en aplicaciones de comunicaciones ópticas de alta velocidad, como en redes de ár= ea amplia (WAN), sistemas de transmisión de datos a larga distancia y enlaces submarinos de fibra óptica. Su diseño avanzado y sus propiedades únicas las convierten en una opción preferida para aplicaciones donde se requiere una transmisión de datos eficiente y = confiable en condiciones desafiantes (Radicelli et al., 2019).

Fen&oac= ute;meno de dispersión por PMD

La dispersión por modo de polarización (PMD) es un fenóme= no intrínseco de las fibras ópticas que afecta la integridad de = la señal luminosa transmitida. Ocurre debido a las variaciones en la velocidad de propagación de los diferentes modos de polarizaci&oacut= e;n de la luz a lo largo de la fibra. Estas variaciones pueden deberse a asimetrías en la estructura de la fibra, tensiones mecánicas,= imperfecciones en el material o fluctuaciones en el índice de refracción a lo largo de la fibra (Qureshi, 2020).

La relación entre la PMD y las fibras ópticas es crucial para comprender cómo se comporta la luz en estos medios de transmisi&oacu= te;n y cómo se ve afectada su calidad. La PMD puede causar distorsiones temporales en la señal luminosa, lo que resulta en el alargamiento y ensanchamiento del pulso óptico. Esto puede provocar la superposición de pulsos vecinos y dificultar la correcta interpretación de la información transmitida.

Las fibras ópticas son particularmente susceptibles a la PMD en situacio= nes donde se requiere una alta tasa de transferencia de datos y/o largas distan= cias de transmisión. En las fibras de índice gradual con dispersión no nula de la velocidad de grupo (NZDSF), como las estudi= adas en esta investigación, la PMD puede ser un factor limitante en el rendimiento de los sistemas de comunicación óptica, ya que es= tas fibras están diseñadas para transmitir señales de alta velocidad y larga distancia (Revelo, 2019).

Por lo tanto, entender cómo la PMD afecta la transmisión de datos= a través de las fibras ópticas es fundamental para optimizar el diseño y funcionamiento de los sistemas de comunicación óptica. Esto incluye desarrollar técnicas de compensaci&oacut= e;n y mitigación de la PMD, así como diseñar fibras ópticas con características que minimicen su impacto. La investigación en este campo contribuye al avance de las tecnologías de comunicación óptica y al desarrollo de redes más eficientes y confiables.

Est&aac= ute;ndar ITU-T G.655 y herramientas de simulación óptica

El estándar ITU-T G.655, desarrollado por la Unión Internacional= de Telecomunicaciones (ITU-T), es un conjunto de especificaciones que define l= as características de las fibras ópticas de dispersión desplazada no nula (NZDSF) utilizadas en sistemas de comunicaciones ópticas de alta velocidad y larga distancia. Este estándar establece los parámetros clave de diseño y rendimiento de las fibras ópticas NZDSF para garantizar su interoperabilidad y compatibilidad en las redes de telecomunicaciones (Navarro et al., 2020).

El ITU-T G.655 especifica diversos parámetros, incluyendo la dispersión cromática, la dispersión de la velocidad de grupo, la atenuación, la longitud de onda de operación y otros aspectos relacionados con las características ópticas y mecánicas de las fibras ópticas NZDSF. Estos parámetros son críticos para garantizar una transmisión eficiente y confiable de datos a través de las fibras ópticas en entornos= de comunicaciones de alta velocidad (Peñaranda & Rodríguez, = 2019).

El estándar ITU-T G.655 ha sido fundamental para el desarrollo y despli= egue de redes de comunicaciones ópticas avanzadas en todo el mundo. Al establecer especificaciones uniformes y rigurosas para las fibras ópticas NZDSF, el estándar garantiza que los equipos de telecomunicaciones de diferentes fabricantes puedan interoperar de manera efectiva y que las redes puedan operar de manera confiable y eficiente (San= i, 2022).

Las herramientas de simulación óptica desempeñan un papel crucial en el diseño, análisis y optimización de siste= mas de comunicaciones ópticas. OptiSystem, en particular, es una platafo= rma de simulación óptica ampliamente utilizada en la industria y = la investigación para modelar y evaluar el rendimiento de sistemas ópticos en diversas aplicaciones.

OptiSystem ofrece una amplia gama de componentes y módulos que permiten simular= con precisión diferentes aspectos de los sistemas de comunicaciones ópticas, como fuentes de luz, fibras ópticas, dispositivos de modulación y demodulación, amplificadores ópticos, y detectores. Esta versatilidad y flexibilidad hacen de OptiSystem una herramienta poderosa para investigadores y profesionales que buscan compren= der y optimizar el comportamiento de los sistemas ópticos en condiciones diversas y realistas (Selvendran et al., 2019).

En el contexto de esta investigación sobre la dispersión por mod= o de polarización (PMD) en fibras ópticas NZDSF según el estándar ITU-T G.655, OptiSystem fue una herramienta fundamental para simular y analizar el comportamiento de las señales ópticas en condiciones específicas. Permitió modelar con precisión los efectos de la dispersión por PMD en las señales de luz qu= e se propagan a través de las fibras ópticas NZDSF, considerando diversos parámetros como la longitud de la fibra, la velocidad de transmisión y el coeficiente de PMD.

Mediante simulaciones realizadas en OptiSystem, fue posible evaluar el impacto de la dispersión por PMD en el rendimiento de los sistemas de comunicacion= es ópticas y analizar cómo afecta a la calidad de la seña= l, la atenuación y otros parámetros importantes. Estas simulacio= nes proporcionaron información valiosa para comprender mejor el fenómeno de la PMD y para diseñar estrategias de compensación que puedan mitigar sus efectos en las redes de comunica= ciones ópticas (Vergel & Acosta, 2022).

&n= bsp;

Metodol= ogía

La metodología utilizada en este estudio se basó en la simulación de la dispersión por modo de polarización (= PMD) en fibras ópticas NZDSF según el estándar ITU-T G.655, utilizando el software OptiSystem. Se configuró el mód= ulo Optical Fiber de OptiSystem para replicar fibras ópticas NZDSF, permitie= ndo la variación de sus parámetros y características para = una simulación precisa.

Se prestó especial atención a los valores especificados en la recomendación ITU-T G.655 sobre el coeficiente de PMD, con el objeti= vo de simular de manera precisa la propagación de pulsos a travé= s de una fibra NZDSF. Se explicaron conceptos clave relacionados con el coeficie= nte de PMD y se definieron los escenarios de simulación, incluyendo valo= res de PMD y distancias específicas, de acuerdo con los requisitos de la investigación.

Se llevó a cabo un análisis inicial de la capacidad de transmisión de datos en diferentes longitudes de onda y valores de P= MD a una distancia fija de 2000 km. Posteriormente, se realizaron simulaciones adicionales con compensadores de PMD para evaluar su efecto en la capacidad= de transmisión de datos a diversas distancias.

Estos escenarios de simulación proporcionaron información detallada sobre el impacto de la dispersión por modo de polarización en= la transmisión de pulsos ópticos a través de fibras ópticas NZDSF, lo que permitió validar la teoría expue= sta en la investigación. Los resultados obtenidos fueron analizados y comparados para obtener conclusiones significativas sobre el comportamiento= de la dispersión por modo de polarización en fibras óptic= as NZDSF.

Tabla 1

Escenarios de simulación

Análisis Inicial

PMD 1

0.1

PMD 2

0.3

Datos

Ventana

Distancia

Gbps

1310

 

 

2000 Km

10

1400

40

1550

80

1610

140

 =

Resulta= dos

La dispersión por modo de polarización (PMD) en fibras ópticas es un fenómeno que afecta la calidad de la transmisión de señales, especialmente en sistemas de alta velocidad. La fibra óptica NZDSF (Non-Zero Dispersion Shifted Fib= er), normada bajo la recomendación ITU-T G.655, ofrece un perfil de dispersión diseñado para minimizar los efectos de la dispersión cromática, pero aún puede estar sujeta a PM= D, lo que influye en la integridad de los datos transmitidos. En este estudio,= se explora el comportamiento de la PMD en fibras NZDSF, analizando su impacto = en la transmisión de señales y evaluando el cumplimiento con las especificaciones de la ITU-T G.655. A continuación, se presentan los resultados obtenidos, que revelan tanto las ventajas como las limitaciones = de este tipo de fibra en aplicaciones de telecomunicaciones de alta velocidad.=

  1.  Entorno de simulación <= o:p>

Para esta simulación, se han utilizado valores estándar de coefici= ente de Dispersión por Modo de Polarización (PMD) de 0.3 y 0.1 ps/= km^1/2, que son comunes en la industria de fibras ópticas comerciales. Estos valores están en línea con las especificaciones de la recomendación ITU-T G.655 para diversas categorías de fibras.= La selección de estos valores comerciales garantiza la aplicabilidad de= los escenarios simulados en una amplia variedad de aplicaciones y entornos de f= ibra óptica, sin limitarse a un tipo específico de uso.=

b.&n= bsp;      Análisis de la simulación de PMD

La tabla 2 resume los resultados de las simulaciones realizadas en varios esce= narios, mostrando la relación entre el porcentaje de atenuación y el factor Q para diferentes valores de PMD. Estos resultados ofrecen una visión clara de los niveles de atenuación y dispersión asociados con cada valor de PMD, resaltando el factor Q máximo como = un indicador crucial de la calidad de la transmisión. Se identificarán dos casos significativos para cada valor de PMD: uno representando las condiciones más críticas de degradaci&oacut= e;n de la señal y otro reflejando condiciones más estables y favorables para la transmisión.

Tabla 2

Resumen de resultados de la simulación<= /p>

PMD

Vtx

nm

Atenuación (%)<= /o:p>

Factor Q<= /i>

0,1ps/(km^0,5)

10

1310

0-2

284,203

1400

0al2

283,824

1550

0al2

284,491

1610

0-2

283.796

40

1310

0al5

140,929

1400

0al8

140,598

1550

0al8

140,162

1610

10al20

141.105

80

1310

30al50

91,0193

1400

30al60

91,0193

Tabla 2

Resumen de resultados de la simulación (continuación)<= o:p>

PMD

Vtx

nm

Atenuación (%)<= /o:p>

Factor Q<= /i>

0,1ps/(km^0,5)

1550

10al25

91,5009

1610

10al20

87,5143

120

1310

30al50

49,1564

1400

50al70

49,5912

1550

25-50

73,1931

1610

30-60

52,3588

0,3ps/(km^0,5)

10

1310

0al8

283,384

1400

5al15

274,631

1550

0al2

283,649

1610

5al10

275,481

40

1310

30al60

126,151

1400

20al35

91,3383

1550

20al40

126,752

1610

30al50

122,188

80

1310

30al60

54,6505

1400

40al70

56,8536

1550

30al60

64,5415

1610

50al70

51,0609

120

1310

50al80

30,0641

1400

70-95

0

1550

70al90

30,7889

1610

70-100

36,5677

&n= bsp;

Se han seleccionado cuatro casos significativos de la tabla de resultados para= un análisis más detallado. En primer lugar, se destaca el caso c= on PMD =3D 0,1 ps/km^ (1/2) y factor Q máximo, representando condiciones óptimas de transmisión con una atenuación mínim= a y una dispersión controlada. En contraste, el caso con PMD =3D 0,1 ps/= km^ (1/2) y factor Q mínimo refleja condiciones desfavorables con una alta atenuación y dispersión.

Para el valor de PMD =3D 0,3 ps/km^ (1/2), el caso con factor Q máximo mu= estra una atenuación aceptable pero una dispersión significativa, mientras que el caso con factor Q mínimo revela una alta atenuación y dispersión, indicando condiciones críticas para la transmisión. Estos cuatro casos proporcionan una visió= ;n equilibrada de cómo varían la atenuación y la dispersión en función de diferentes valores de PMD y factores= Q, siendo útiles para evaluar la eficacia de las técnicas de compensación y optimización en la transmisión de señales ópticas.

c.&n= bsp;       Simulación pre-compensadora de PMD

·         Caso 1 (1400nm; L=3D1000 Km; Vtx=3D120 Gbps; φPMD =3D 0,3 ps/km^1/2): Ligera mejora en dispersión pero no suficiente para una compensación efectiva. La atenuación y la dispersión siguen siendo altas, lo que indica limitaciones en la efectividad del pre compensador.

·         Caso 2 (1400nm; L=3D2000 Km; Vtx=3D40 Gbps; &= #966;PMD =3D 0,3 ps/km^1/2): Leve mejora en atenuación. Se observa una mejora en la calidad de la transmisión y la estabilidad de la señal.

·         Caso 3 (1400nm; L=3D5000 Km; Vtx=3D10 Gbps; &= #966;PMD =3D 0,3 ps/km^1/2): Mejora significativa en atenuación y dispersión después de la compensación. La transmisión se vuelve más estable y confiable, con una menor pérdida de potencia de la señal.

·         Caso 4 (1550nm; L=3D1000 Km; Vtx=3D120 Gbps; φPMD =3D 0,3 ps/km^1/2): Compensación no efectiva. No se obser= va una mejora significativa en atenuación y dispersión después de la aplicación del pre compensador.

El caso más significativo al usar el pre compensador sería el Ca= so 3 (1400nm; L=3D5000 Km; Vtx=3D10 Gbps; φPMD =3D 0,3 ps/km^1/2), ya que m= uestra una mejora significativa en atenuación y dispersión despué= s de la compensación como se muestra en la figura 1 y 2. Esto indica una transmisión más estable y confiable, lo que resalta la efectividad del pre compensador en este escenario específico.

Figura = 1        =             &nb= sp;            =             &nb= sp;         &= nbsp;          Figura 2

Pre-com= pensación para dos pulsos a 10 Gbps   Dos análisis cadenas de cara= cteres a 10   Gbps

3D"Gráfico

Descripción3D"Imagen

d.&n= bsp;      Simulación post-compensadora de PMD

·         Caso 1 (1400nm; L=3D1000 Km; Vtx=3D120 Gbps; φPMD =3D 0,3 ps/km^1/2): Ligera mejora en la atenuación, pero = sin impacto significativo en la dispersión. El post compensador muestra = una efectividad limitada en este caso, con una mejora marginal en la transmisión de la señal.

·         Caso 2 (1400nm; L=3D2000 Km; Vtx=3D40 Gbps; &= #966;PMD =3D 0,3 ps/km^1/2): Notable mejora en la dispersión, mientras = que la atenuación se mantiene. La eficacia del post compensador se obser= va en la mejora de la calidad de la transmisión al abordar los efectos = de dispersión.

·         Caso 3 (1400nm; L=3D5000 Km; Vtx=3D10 Gbps; &= #966;PMD =3D 0,3 ps/km^1/2): Mejora significativa en dispersión sin comprometer la atenuación. El post compensador demuestra su eficienc= ia al mitigar los efectos de dispersión sin introducir pérdidas = adicionales.

·         Caso 4 (1550nm; L=3D1000 Km; Vtx=3D120 Gbps; φPMD =3D 0,3 ps/km^1/2): Mejora notable en la atenuación, pero= la dispersión se mantiene. Mientras se observa una mejora en la atenuación, la efectividad del post compensador en la dispersi&oacut= e;n es limitada, sugiriendo la necesidad de ajustes adicionales.

El caso más significativo al usar el post compensador sería el C= aso 3 (1400nm; L=3D5000 Km; Vtx=3D10 Gbps; φPMD =3D 0,3 ps/km^1/2), ya que= muestra una mejora significativa en la dispersión sin comprometer la atenuac= ión como indica la figura 3 y 4. Esto indica una transmisión más confiable y estable, destacando la eficacia del post compensador en este escenario específico.

Figura = 3        =             &nb= sp;            =             &nb= sp;            =         Figura 4

Dos mue= stras bajo las mismas condiciones  &nbs= p;            &= nbsp; Dos muestras de una cadena de caracteres en el post-compensador        &= nbsp;           &nbs= p;            &= nbsp; bajo las mismas condiciones

3D"Gráfico

Descripción    3D"Diagrama

Descripción

 

 

Conclusiones

·  &n= bsp;      Los resultados de las simulaciones utilizando tanto pre compensadores como post compensadores revelan la complejidad y la importancia de abordar los efectos de dispersión por modo de polarización (PMD) en sistemas de comunicación óptica.= Si bien ambos enfoques muestran mejoras en la transmisión de la señal en ciertos casos, la eficacia varía considerablemente dependiendo de factores como la longitud de onda, la distancia de transmisión y la velocidad de transmisión. =

·         En particular, los posts compensadores muestran promesa al mitigar los efectos de dispersión en algunos escenarios, destacando su papel en mejorar la calidad y la confiabilidad de la transmisión óptica. Sin embargo, se requiere un anális= is más detallado y ajustes adicionales para optimizar la eficacia de es= tos dispositivos en entornos específicos de comunicación óptica. Estos hallazgos subrayan la necesidad de una aproximaci&oacu= te;n cuidadosa y adaptativa al abordar los desafíos de dispersión = en sistemas de fibra óptica para garantizar un rendimiento óptim= o en una amplia gama de condiciones operativas.

Conflicto de intereses

Los aut= ores declaran que no existe conflicto de intereses en relación con el artíc= ulo presentado.

Referencias Bibliográficas=

Alustiz= a, D., Mineo, M., Aredes, D., & Russo, N. (2019). Fabricación local de sensores de fibra óptica aplicables al sensado de magnitudes relevan= tes en ingeniería civil. Ingenio Tecnológico Revista de Ingeni= ería, 1(1), 1-10. http://sedici.unlp.edu.ar/handle/10915/153462=

Cadena, Jorge, & Jiménez, María Soledad. (2019). Análisis y Simulación del Fenómeno de Dispersión por Modo de Polarización (PMD) en Fibras Ópticas ITU-T G.655.= Revista Politécnica, 43(2), 21-28. http://scielo.senescyt.gob.ec/scielo.php?script= =3Dsci_arttext&pid=3DS1390-01292019000300021&lng=3Des&tlng=3Des= .

Chepkoi= wo, H., Mwaura, K., Wafula, D., Rotich, E., Kiboi, D., Mosoti, G., Leitch, A., & Gibbon, T. (2020). Performance of 1550 nm VCSEL at 10 Gb/s in G.655 and G.652 SSMF. International Journal of Sustainability Management and Information Technologies, 6(1), 13-17. https://doi.org/10.11648/j.ijsmit.20200601.12<= /o:p>

Cot&iac= ute; Aceytuno, J. (2022). Diseño de investigación de una aplicación móvil para el control del desarrollo de ATP de proyectos en planta externa de anillos principales core de fibra ópt= ica en una empresa de telecomunicaciones [Tesis de pregrado, Universidad de San Carlos de Guatemala, Guatemala]. http://= www.repositorio.usac.edu.gt/19193/

Landivar, Mirko. (2021). Acoplami= ento de la electrodinámica de Maxwell-Chern-Simons a un campo gravitacion= al en presencia de un medio óptico no dispersivo en 2+1 dimensiones. Revista Boliviana de Física, 39(39), 10-16. http://www.scielo.org.bo/scielo.php?script=3Dsci_arttext&pid=3DS1562-38= 232021000200003&lng=3Des&tlng=3Des.

Navarro Restrepo, J. D., Rojas Úsuga, J., Martínez Cir= o, R., Betancur Pérez, A., y López Giraldo, F. (2020). Caracterización de un conversor de luz a frecuencia TSL235R-LF, para= su aplicación en un sistema de comunicación por luz visible. = Revista EIA, 17(34), 1–7. https://doi.org/10.24050/reia.v17i34.113= 9

Pe&ntil= de;aranda, M., & Rodríguez, P. (2019). Diseño de fibras óptic= as con dispersión modificada. https://www.academia.edu/55295370/Dise%C3= %B1o_De_Fibras_%C3%93pticas_Con_Dispersi%C3%B3n_Modificada

Radicel= li, C., Pomboza, M., Samaniego, N., & Villacrés, E. (2019). Red óptica pasiva para proveer de Internet a la ciudad de Riobamba. Espacios, 40(40), 12-20. http://obsinvestigacion.unach.edu.ec/sccitys/m= od_ob/admin/news.jsp?codid=3D2396

= Qureshi, K. K., Qu= reshi, A. R., Magam, M. G., & Jamal, L. (2023). Radio-over-fiber front-haul link design using Opti system. Journal of Optical Communications, 44(1), 1297-1303. https://doi.org/10.1515/joc-2020-0074=

Revelo Aldas, M. D. (2019). Análisis de normativas para redes GPON y la calidad de servic= io en Ecuador. Recinat= ur International Journal of Applied Sciences, Nature and Tourism, 1(1), 1-12.  https://rev= istasojs.utn.edu.ec/index.php/recinatur/article/view/389<= span lang=3DEN-US style=3D'font-size:12.0pt;line-height:115%'>=

Sánchez Nieto, A. G., Rubén Ramírez Ramírez, C., Guzmán Magaña, A., Constantino Herrera, J. A., López Guzmán, K., Ledesma Carrillo, L. M., & Mata Chávez, R. I. (2023). Análisis de= un patrón de moteado de fibra óptica plástica con procesa= miento digital de imágenes. Jóvenes en la Ciencia, 21, 1–10. https://www.jovenesenlaciencia.ugto.mx/index.php/jovenesenlaciencia/article= /view/3995

Sani Domínguez, J. E. (2022). Diseño, evaluación de una red FTTH utilizando Optisystem y estrategia para la obtención de concesión que permita brindar servicios triples = play [Tesis de maestría, Escuela Superior Politécnica de Chimboraz= o. Riobamba, Ecuador]. <= span style=3D'font-size:12.0pt;line-height:115%;mso-ansi-language:ES-EC'>http://= dspace.espoch.edu.ec/handle/123456789/15713

Selvendran, S., Raja, A. S., Muthu, K. E., & Lakshmi, A. (2019). Certain Investigation on Visible Light Communication with OFDM Modula= ted White LED Using Optisystem Simulation. Wireless Personal Communications<= /span>, 10= 9(2), 1377-1394. https://doi.org/10.1007/s11277-019-06617-2

Vergel Cazorla, F. E., & Acosta Mejía, A. F. (2022). Estudio y análisis de las atenuaciones y potencias ópticas para la optimización del presupuesto óptico mediante pruebas en una RED FTTH en el Cant&oacut= e;n Durán sector Los Helechos [Tesis de pregrado, Universidad de Guayaquil, Guayaquil, Ecuador]. http://repositorio.ug.ed= u.ec/handle/redug/59845

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El artículo que se publica es de exclusiva responsabilidad de los autores y no necesariamente reflejan el pensamiento de la Revista Alfa Publicaciones.

&nbs= p;

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El artículo queda en propiedad de la revist= a y, por tanto, su publicación parcial y/o total en otro medio tiene que = ser autorizado por el director de la R= evista Alfa Publicaciones.

 

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//////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// /////////////////////////////////////////////////////////////////////wAAAAD/ //8AAAD///////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////8AAAAA////AAAA//////////////////////////// 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//////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////8AAAAA////AAAA//////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// ////////////////////////////////////////////////////////////////////////AAAA AP///wAAAP////////////////////////////////////////////////////////////////// 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//////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////8AAAAA////AAAA//////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// 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//////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// /////////////////////////////wAAAAD///8AAAD///////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////8AAAAA 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//////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////8AAAAA////AAAA//////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// ////////AAAAAP///wAAAP////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// /////////////////////////////////////////////////wAAAAD///8AAAD///////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////8AAAAA////AAAA//////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// ////////////////////////////////////////////////////////AAAAAP///wAAAP////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// /////////////////////wAAAAD///8AAAD///////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////8AAAAA////AAAA //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// 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/////////////////////////////////////////////////////////////////////wAAAAD/ //8AAAD///////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////8AAAAA////AAAA//////////////////////////// //////////////////////////////////////////////////////////////////////////// //////////////////////////////////////////////////////////////////////////// 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