Lecture 3 Optical fibers

Slides:



Advertisements
Similar presentations
Unit-2 Polarization and Dispersion
Advertisements

Waveguides Part 2 Rectangular Waveguides Dielectric Waveguide
S Digital Communication Systems Fiber-optic Communications - Supplementary.
PROPAGATION OF SIGNALS IN OPTICAL FIBER 9/13/11. Summary See notes.
Nonlinear Optics Lab. Hanyang Univ. Chapter 3. Propagation of Optical Beams in Fibers 3.0 Introduction Optical fibers  Optical communication - Minimal.
EE 230: Optical Fiber Communication Lecture 5 From the movie Warriors of the Net Attenuation in Optical Fibers.
The Optical Fiber and Light Wave Propagation Xavier Fernando Ryerson Comm. Lab.
Optical Fiber Basics Part-3
1 Lecture 5b Fiber-Optics in Digital Communication Systems & Electronic Interfaces 1. Introduction 2.Geometric Optics 3.Classification of Optical Fibers.
EE 230: Optical Fiber Communication Lecture 2 From the movie Warriors of the Net Fibers from the view of Geometrical Optics.
EE 230: Optical Fiber Communication Lecture 6 From the movie Warriors of the Net Nonlinear Processes in Optical Fibers.
EE 230: Optical Fiber Communication Lecture 3 Waveguide/Fiber Modes From the movie Warriors of the Net.
EE 230: Optical Fiber Communication Lecture 4
Tutorial on optical fibres F. Reynaud IRCOM Limoges Équipe optique F. Reynaud IRCOM Limoges Équipe optique Cargèse sept 2002.
Lecture 1 Review of Wave optics Today Introduction to this course Light waves in homogeneous medium Monochromatic Waves in inhomogeneous medium.
Lecture 4b Fiber Optics Communication Link 1. Introduction 2
Dispersion Measurements Lecture-3. Dispersion Measurements Measurement of Intermodal Dispersion The most common method for measuring multimode fiber bandwidth.
Fiber-Optic Communications
System Performance Stephen Schultz Fiber Optics Fall 2005.
1 Stephen SchultzFiber Optics Fall Optical Fibers.
L5 Optical Fiber Link and LAN Design
Service d’Électromagnétisme et de Télécommunications 1 1 Attenuation in optical fibres 5 ème Electricité - Télécommunications II Marc Wuilpart Réseaux.
Fiber Optics Communications Lecture 11. Signal Degradation In Optical Fibers We will look at Loss and attenuation mechanism Distortion of optical signals.
Propagation of Signals in Optical Fiber
Optical Fiber Basics-Part 2
ENE 429 Antenna and Transmission lines Theory Lecture 9 Optical fiber DATE: 04/09/06 08/09/06.
FIBER PROPERTIES Transmission characteristics of a fiber depends on two important phenomena Attenuation Dispersion Attenuation or transmission loss Much.
9/12/  Most optical fibers are used for transmitting information over long distances.  Two major advantages of fiber: (1) wide bandwidth and (2)
9/12/  Most optical fibers are used for transmitting information over long distances.  Two major advantages of fiber: (1) wide bandwidth.
PROPAGATION OF SIGNALS IN OPTICAL FIBER 9/20/11. Light Characteristics Particle Characteristics Light has energy Photons are the smallest quantity of.
Optical Fibre Communication Systems
Opto Electronics Lecturer # 04 Fiber Loses. Lecturer objective Basic causes of fiber energy loss and dispersion Fiber energy loss and dispersion, effect.
Intermode Dispersion (MMF)
For single mode operation, V = (2a/)(n12n22 )1/2 2.405
Chapter 4: Optical fibers and their parameters Graphic representation of three different types of how the refractive index change in the core of an optical.
Optical Fiber Communications
Optical Fibre Dispersion By: Mr. Gaurav Verma Asst. Prof. ECE NIEC.
FIBER OPTICS. Increase in Bitrate-Distance Product Agrawal-Fiber Optic Communications.
LOSSES IN FIBER OPTIC SYSTEM
§2 Optical Fibres – a brief introduction Anatomy of a Fiber Cable Fig. 2.1: Anatomy of a fiber.
Discrete optics v.s. Integrated optics
Review First Exam What have we learned? Any traveling sinusoidal wave may be described by y = y m sin(kx   t +  ) Light always reflects with an angle.
UNIT II TRANSMISSION CHARACTERISTICS OF OPTICAL FIBERS Dr.Gnanasundari/Prof/ECE/SNSCE/OCN/Unit II.
1 OPTICAL COMMUNICATIONS S Course Program 5 lectures on Fridays  First lecture Friday in Room H-402  13:15-16:30 (15 minutes break.
Propagation of Light Through Optical Fiber. Outline of Talk Acceptance angle Numerical aperture Dispersion Attenuation.
Lecture 4. Pulse Propagation in Fibers Problem: Inject an optical pulse of width  0 into the fiber at z = 0. What is the speed of propagation and what.
Chapter 3 Signal Degradation in Optical Fibers
S Digital Communication Systems Overview into Fiber Optic Communications.
Optical Communication et4-013 B1 Optical Communication Systems Opto-Electronic Devices Group Delft University of Technology Opto-Electronic Devices Group.
Transmission Characteristic of Optical Fibers
OPTICAL FIBER COMMUNICATION
Phase velocity. Phase and group velocity Group velocity.
UPM, DIAC. Open Course. March TIME DISPERSION 3.1 Introduction 3.2 Modal Dispersion 3.3 Chromatic Dispersion 3.4 PMD 3.5 Total Dispersion 3.6 Dispersion.
CHAPTER 2 Dielectric Waveguides and Optical Fibers
Chapter XII Propagation of Optical Beams in Fibers
Chapter 3 Signal Degradation in Optical Fibers
Optical Fiber Basics Part-3
OPTICAL FIBRE BASED ON MODES (OR) MODE TYPES
GROUP DELAY Group delay per unit length can be defined as:
Optical Fiber.
The Optical Fiber and Light Wave Propagation
SIGNAL DISTORTION IN OPTICAL WAVE GUIDES
Mode coupling in optic fibers
Chapter 3: Optical Devices Optical Fibers
The University of Adelaide, School of Computer Science
Optical Fiber Communication
COMMUNICATION ENG. PROF. A.M.ALLAM
NET 436 optical Network Tutorial Lecture #2
COMMUNICATION ENG. PROF. A.M.ALLAM
COMMUNICATION ENG. PROF. A.M.ALLAM
Presentation transcript:

16.711 Lecture 3 Optical fibers Last lecture Geometric optic view of waveguide, numeric aperture Symmetric planar dielectric Slab waveguide Modal and waveguide dispersion in palnar waveguide Rectangular waveguide, effective index method

16.711 Lecture 3 Optical fibers Today Fiber modes Fiber Losses Dispersion in single-mode fibers Dispersion induced limitations Dispersion management The Graded index fibers

16.711 Lecture 3 Optical fibers Fiber modes --- single mode and multi-mode fibers V-number Number of modes when V>>2.41 Normalized propagation constant for V between 1.5 – 2.5. Mode field diameter (MFD)

16.711 Lecture 3 Optical fibers Examples --- single mode and multi-mode fibers 1. Calculate the number of allowed modes in a multimode step index fiber, a = 100 m, core index of 1.468 and a cladding index of 1.447 at the wavelength of 850nm. Solution: 2. What should be the core radius of a single mode fiber that has the core index of 1.468 and the cladding index of 1.447 at the wavelength of 1.3m. Solution: a < 2.1m 3. Calculate the mode field diameter of a single mode fiber that has the core index of 1.458 and the cladding index of 1.452 at the wavelength of 1.3m. Solution:

16.711 Lecture 3 Optical fibers Fiber loss Material absorption silica electron resonance <0.4m OH vibrational resonance ~ 2.73 m Harmonic and combination tones ~1.39 m 1.24 m, 0.95 m Rayleigh scattering Local microscopic fluctuations in density C~ 0.8dB/km m4 0.14dB loss @ 1.55m Bending loss and Bending radius

16.711 Lecture 3 Optical fibers Dispersions in single mode fiber Material dispersion Example --- material dispersion Calculate the material dispersion effect for LED with line width of 100nm and a laser with a line width of 2nm for a fiber with dispersion coefficient of Dm = 22pskm-1nm-1 at 1310nm. Solution: for the LED for the Laser

16.711 Lecture 3 Optical fibers Dispersions in single mode fiber Waveguide dispersion Example --- waveguide dispersion n2 = 1.48, and delta n = 0.2 percent. Calculate Dw at 1310nm. Solution: for V between 1.5 – 2.5.

16.711 Lecture 3 Optical fibers chromatic dispersion (material plus waveduide dispersion) material dispersion is determined by the material composition of a fiber. waveguide dispersion is determined by the waveguide index profile of a fiber

16.711 Lecture 3 Optical fibers Polarization mode dispersion fiber is not perfectly symmetric, inhomogeneous. refractive index is not isotropic. dispersion flattened fibers: Use waveguide geometry and index profiles to compensate the material dispersion

16.711 Lecture 3 Optical fibers Dispersion induced limitations For RZ bit With no intersymbol interference For NRZ bit With no intersymbol interference

16.711 Lecture 3 Optical fibers Dispersion induced limitations Optical and Electrical Bandwidth Bandwidth length product

16.711 Lecture 3 Optical fibers Dispersion induced limitations Example --- bit rate and bandwidth Calculate the bandwidth and length product for an optical fiber with chromatic dispersion coefficient 8pskm-1nm-1 and optical bandwidth for 10km of this kind of fiber and linewidth of 2nm. Solution: Fiber limiting factor absorption or dispersion?

16.711 Lecture 3 Optical fibers Dispersion Management Pre compensation schemes Prechirp Gaussian Pulse:

16.711 Lecture 3 Optical fibers Dispersion Management Pre compensation schemes Prechirp Prechirped Gaussian Pulse:

16.711 Lecture 3 Optical fibers Dispersion Management Prechirp With T1/T0 = sqrt(2), the transmission distance is:

16.711 Lecture 3 Optical fibers Dispersion Management Examples: 1. What’s the dispersion limited transmission distance for a 1.55m light wave system making use of direct modulation at 10Gb/s? D = 17ps(km-nm). Assume that frequency chirping broadens the guassian-shape by a factor of 6 from its transform limited width. Solution:

16.711 Lecture 3 Optical fibers Dispersion compensation fiber or dispersion shifted fiber Why dispersion compensation fiber: for long haul fiber optic communication. All–optical solution Approaches longer wavelength has a larger index. make the waveguide weakly guided so that longer wavelength has a lower index.

16.711 Lecture 3 Optical fibers The Graded index fibers Approaches Only valid for paraxial approximation General case Intermode dispersion Calculate the BL product of a grade index filber of 50m core with refractive index of n1 = 1.480 and n2 = 1.460. At 1.3 m. Solution: