Lasers & Fiber Optics Engr. Hyder Bux Mangrio Engr. Fayaz Hassan Mangrio 1 Introduction L&FO labs • • • • • • • Lab #01: Introduction to Fiber optics Communication System Lab #02: Optical Sources Lab #03: Optical Detectors Lab #04: Optical fiber attenuation losses Lab #05: Analog voice transmission Lab #06: Understanding basic function of S122A splicer Lab #07: Perform Fusion/Mechanical Splicing 2 Introduction • • • • • Lab #08: Understanding the basic function of OTDR Lab #09: Perform fiber measurement on OTDR Lab #10: Fiber attenuation measurement using Cut-Back method Lab #11: Optical Field Spectrum Analyzer Lab #12: Overview of Power meter & Light Source 3 Information • Email: hyder.bux@faculty.muet.edu.pk • Webpage: https://sites.google.com/a/faculty.muet.edu.pk/hyder mangrio/ • Optical Communication Laboratory • Consultation Timings: Monday(8am to 3pm) & Friday (8am to 1pm) 4 Laboratory • There will be at least 13 labs covering in 13 weeks course. Each lab will be approximately 2 hours long. The lab report / Handout is due to the lab assistant before next lab. 5 What is lightwave technology? • Lightwave technology uses light as the primary medium to carry information. • The light often is guided through optical fibers (fiberoptic technology). • Most applications use invisible (infrared) light. (HP) Why lightwave technology? • Most cost-effective way to move huge amounts of information (voice, data) quickly and reliably. • Light is insensitive to electrical interference. • Fiber optic cables have less weight and consume less space than equivalent electrical links. (HP) Use Of Lightwave Technology • Majority applications: – Telephone networks – Data communication systems – Cable TV distribution • Niche applications: – Optical sensors – Medical equipment LW Transmission Bands 193 Frequency Wavelength (vacuum) Longhaul Telecom Regional Telecom Local Area Networks 229 353 461 THz Near Infrared 1.8 1.6 1.4 1.2 UV 1.0 0.8 0.6 0.4 HeNe Lasers 633 nm 1550 nm CD Players 780 nm 1310 nm 850 nm 0.2 µm Introduction to Fiber Optics • Fiber optics is a medium for carrying information from one point to another in the form of light. Unlike the copper form of transmission, fiber optics is not electrical in nature. • A basic fiber optic system consists of a transmitting device that converts an electrical signal into a light signal, an optical fiber cable that carries the light, and a receiver that accepts the light signal and converts it back into an electrical signal. 10 Introduction to fiber Optics 11 Optical Sources • Two main types of optical sources – Light emitting diode (LED) • Large wavelength content • Incoherent • Limited directionality – Laser diode (LD) • Small wavelength content • Highly coherent • Directional 12 Light Emitting Diodes (LED) • Spontaneous emission dominates – Random photon emission • Spatial implications of random emission – Broad far field emission pattern – Dome used to extract more of the light • Spectral implications of random emission – Broad spectrum Laser Diode • Stimulated emission dominates – Narrower spectrum – More directional • Requires high optical power density in the gain region – Optical Feedback: Part of the optical power is reflected back into the cavity – End mirrors • Lasing requires net positive gain – Cavity gain • Depends on external pumping • Applying current to a semiconductor pn junction – Cavity loss • Material absorption • Scatter • End face reflectivity Optical Detectors • Inverse device with semiconductor lasers – Source: convert electric current to optical power – Detector: convert optical power to electrical current • Use pin structures similar to lasers • Electrical power is proportional to i2 – Electrical power is proportional to optical power squared – Called square law device • Important characteristics – – – – Modulation bandwidth (response speed) Optical conversion efficiency Noise Area HOW DOES FIBRE OPTIC WORK ? Carries Signals as Light Pulses signals converted from electrical to light (and visaversa) by special equipment e.g. fibre-optic “transceiver” (transmitter / receiver) FIBRE CONSTRUCTION 125 Cladding Glass 8, 50, 62.5 Core Glass PRIMARY BUFFER Primary Buffer 250 Cladding 125 Core (62.5) SECONDARY BUFFER Secondary Buffer 900 Primary Buffer 250 Cladding 125 Core (62.5) FIBRE MATERIAL Silica Glass used for high-speed data applications Plastics used for low-speed data / voice applications Composite Constructions used for low-speed and specialized applications FIBRE TRANSMISSION Multi-Mode graded-index used for short / medium distance applications step-index early fibre type - no longer used Single-Mode a.k.a Mono-Mode used for long-distance / very high-speed applications e.g. cross-country and transatlantic communications LIGHT TRANSMISSION MultiMode Step Index MultiMode Graded Index SingleMode COMMON FIBRE SIZES 50 µm 62.5 µm 125 µm 125 µm MultiMode Graded Index 100 µm 140 µm 8 µm 125 µm SingleMode Advantages/Disadvantages of Fiber Optics • Advantages a) b) c) d) e) f) Enormous potential bandwidth Small size and weight Electrical Isolation Signal security Low transmission loss Potential low cost 24 Advantages/Disadvantages of Fiber Optics • Disadvantages a) b) c) High cost for connector and interfacing Requires specialized and sophisticated tools for maintenance and repairing Higher initial cost in installation 25 Light-Source • • • • • • What is light? Properties of Light. Refractive Index Law of Refraction Law of Reflection Total Internal Reflection 26 Refractive Index • The guidance of the light beam which acts as a transmission channel for information (through the optical fiber) takes place because of the phenomenon of total internal reflection (TIR), which is dependent on the refractive index of the medium. The refractive index (n) of a medium can be written as: 27 Total Internal Reflection • A ray of light incident on a denser medium i.e. n1<n2 According to Snell’s Law and the law of reflection we have n1 sin θ1 =n2 sin θ2 and θ1=θ3 28 Total Internal Reflection • The angle of incidence, for which the angle of refraction is 90º, is known as the critical angle and is denoted by θc .Thus, when θ1=θc =sin-1(n2/n1) θ2=90. When the angle of incidence exceeds the angle of critical (i.e.,θ1>θc), there is no refracted ray and we have total internal reflection. 29 Total Internal Reflection 30