DIGITAL PULSE INTERVAL MODULATION (DPIM) AS AN ALTERNATIVE MODULATION SCHEME FOR FREE SPACE OPTICS (FSO)

Slides:



Advertisements
Similar presentations
MIC-CPE2010, Jordan Optimizing the Performance of Digital Pulse Interval Modulation with Guard Slots for Diffuse Indoor Optical Wireless Links Z. Ghassemlooy.
Advertisements

CH. 4 Transmission Media.
Optical Fiber. Prepared By AbdulRahman AlKhayyat Mohamed Felimban.
The Future of Satellite Communications Joel Klooster ENGR 302 May, 2002.
IEEE LANMAN, June 11th, Multi-channel Communication in Free-Space Optical Networks for the Last-mile Jayasri Akella ECSE Department Rensselaer Polytechnic.
Optical Wireless Communications
Optical Wireless Communications
Berkeley Sensor & Actuator Center Smart dust Active Laser Transmitter (SALT) Matthew Last, Kris Pister Berkeley Sensor and Actuator Center
1 Stephen SchultzEE466 Fall Introduction.
Network Evolution in Coming 10 Years: What's the Future of Network? - Toward Optical Wireless Communications- Fan Bai Sato Laboratory, GITS, Waseda University.
April 2003 Mohit Garg, IIT Bombay 1 Free Space Optical Communication Picture:
ICTON 2007, Rome, Italy The Performance of PPM using Neural Network and Symbol Decoding for Diffused Indoor Optical Wireless Links 1 S. Rajbhandari, Z.
Wireless Optical Networking: An Overview Tim Miller Product Manager Broadband Wireless World ForumFebruary 19, 2001.
The Bright Future of Wireless Communications
Sujan Rajbhandari PGNET Performance of Convolutional Coded Dual Header Pulse Interval Modulation in Infrared Links S. Rajbhandari, Z. Ghassemlooy,
Jayasri Akella Error Analysis of Multi-Hop Free-Space Optical Communication Jayasri Akella, Murat Yuksel, Shiv Kalyanaraman Department of Electrical, Computer.
Connectivity Unlimited TM Wireless Optical Transmission at 10 Gbps and Beyond.
EE 566 Optical Communication Ming Li Free Space Optic (FSO)
IASTED- WOC- Canada 07 1 CONVOLUTIONAL CODED DPIM FOR INDOOR NON-DIFFUSE OPTICAL WIRELESS LINK S. Rajbhandari, Z. Ghassemlooy, N. M. Adibbiat, M. Amiri.
Shivkumar Kalyanaraman Rensselaer Polytechnic Institute 1 Multi-Element Array Antennas for Free-Space Optical (FSO) Networks Jayasri Akella, Murat Yuksel,
EE 566 Optical Communications Free Space Optics An overview Snehil Tiwari
All-optical Fog Sensor for Determining the Fog Visibility Range in Optical Wireless Communication Links Muhammad.
Done by Sarah Hussein 10\05\2012. Trends in modern communication systems place high demands on low power consumption, high-speed transmission, and anti-
Chapter 7 Photonic Transmission Systems (Digital & Analog)
Transmission Media / Channels. Introduction Provides the connection between the transmitter and receiver. 1.Pair of wires – carry electric signal. 2.Optical.
L5 Optical Fiber Link and LAN Design
Copyright © 2002 Terabeam Corporation. All rights reserved. 1 Free Space Optics (FSO) Technology Overview John Schuster Chief Technology Officer Terabeam.
 fiber optics cable and free space optics (FSO). Like fiber optics cable, FSO uses lasers to transmit data, but instead of enclosing the data stream.
Free Space Optics The Bright Future of Wireless Communications.
Review: The application layer. –Network Applications see the network as the abstract provided by the transport layer: Logical full mesh among network end-points.
Why Free Space Optics? What are Free Space Optics? Application to American University.
By Zeyad khudhayer University of Baghdad College of Engineering Electronic & communication department 4 th year.
A System View of Optical Fiber Communication prt.2 AbdulRahman AlKhayyat Mohamed Felimban
© N. Ganesan, Ph.D., All rights reserved. Chapter Electronic and Optical Transmission.
Alternative Communications : Survey and Idea Lee, Gunhee.
Chapter 10 Optical Communication Systems
1/ , Graz, Austria Power Spectral Density of Convolutional Coded Pulse Interval Modulation Z. Ghassemlooy, S. K. Hashemi and M. Amiri Optical Communications.
Patch Panels in the Sky: A Case for Free-Space Optics in Data Centers Navid Hamed Azimi, Himanshu Gupta Vyas Sekar, Samir Das.
Design of an Optical Wireless Transmission Link Student Name: Wen Zu Instructor: Dr.Xavier N. Fernando.
CHAPTER 7 SYSTEM DESIGN. Transmission Types Two types of transmissions: - Link (point to point) - Network -point to multipoint -Mesh -Ring.
ECE 4710: Lecture #36 1 Chapter 8  Chapter 8 : Wired and Wireless Communication Systems  Telephone  Fiber Optic  DSL  Satellite  Digital & Analog.
1/21 Chapter 4 – Transmission Media. 2/21 Overview  guided – copper twisted pair, coaxial cable optical fiber  unguided – wireless; through air, vacuum,
ECE 4710: Lecture #2 1 Frequency  Communication systems often use atmosphere for transmission  “Wireless”  Time-varying Electro-Magnetic (EM) Wave 
Flexible Optical Wireless Links and Nexwork IEEE Communication Magazine. March 2003.
ECE 4710: Lecture #13 1 Bit Synchronization  Synchronization signals are clock-like signals necessary in Rx (or repeater) for detection (or regeneration)
Part 3  Transmission Media & EM Propagations.  Provides the connection between the transmitter and receiver. 1.Pair of wires – carry electric signal.
IV B.tech,ECE ( DATA TRANSMISSION THROUGH LASERS ) Presented By K.Sai Bhargav Ram.
Sujan Rajbhandari LCS Convolutional Coded DPIM for Indoor Optical Wireless Links S. Rajbhandari, N. M. Aldibbiat and Z. Ghassemlooy Optical Communications.
Multi-Objective Optimization for Topology Control in Hybrid FSO/RF Networks Jaime Llorca December 8, 2004.
Design of an Multi-Gbp Optical Wireless Transmission Link EE8114 Student Name: Wen Zu.
WELCOME.
Copyright © 2002 Terabeam Corporation. All rights reserved. 1 Free Space Optics (FSO) Technology Overview Presented by M.sriramulu 08621a0432.
Poster Session at Graduate School Information Fair
LASER COMMUNICATION SYSTEM
S. Rajbhandari, Z. Ghassemlooy, J. Perez, H. Le Minh, M. Ijaz,
A System View of Optical Fiber Communication
Free Space Laser Communications
FREE SPACE OPTICS(FSO)
Subject Name: Optical Fiber Communication Subject Code: 10EC72
Making Networks Light March 29, 2018 Charleston, South Carolina.
OPTICAL WIRELESS BROADBAND – CARRIER GRADE TECHNOLOGY WITHOUT THE LICENSING COST
Mehmet Bilgi University of Nevada, Reno
Free Space Optics (FSO) Technology Overview
A System View of Optical Fiber Communication prt.2
Multi-Objective Optimization for Topology Control in Hybrid FSO/RF Networks Jaime Llorca December 8, 2004.
Optical Wireless Communications
CSCI-1680 Physical Layer Link Layer I
Fiber Optic Transmission
Fibre Optic Transmission
Free Space Optics (FSO) Technology Overview
Presentation transcript:

DIGITAL PULSE INTERVAL MODULATION (DPIM) AS AN ALTERNATIVE MODULATION SCHEME FOR FREE SPACE OPTICS (FSO)

Intro to FSO Intra-city Fiber Optic Links Fiber Optic Cable Most Metropolitan Area Networks are inter-connected through high speed fiber optic links. The speed currently being offered as we all now is around 10Gbps. He is an example of a map of Southern Ontario & Western New York where the fiber optic cables are connecting cities from Syracuse to Ottawa to Toronto.

The Reasoning High-speed Access The Last Mile Problem? Picture taken from: I. I. Kim, B. McArthur, and E. Korevaar, Comparison of laser beam propagation @ 785nm and 1550nm in fog and haze for optical wireless communications, Optical Access Incorporated, San Diego The main issue is high-speed access. An interesting note is that only 5 percent of the buildings in the United States are connected to fiber optic backbone, yet 75 percent of the other buildings are within one mile of fiber, hence the name ‘The Last Mile Problem’. As it can be seen from the diagram, the other building are connected to the fiber optic backbone through T1, ADSL, Cable Technologies through existing underground copper wires but can only achieve speeds ranging from 1.5 MBps – 6 MBps. In order to provide high speed access to the other buildings, fiber optic cables must be buried over the existing copper lines connecting the fiber optic backbone to the buildings. This is a very expensive solution ($10,000/km).

The Solution Free Space Optics Picture taken from: I. I. Kim, and E. Korevaar, Availability of Free Space Optics (FSO) and hybrid FSO/RF systems, Optical Access Incorporated, San Diego Free Space Optics is exactly the same as regular fiber optic communication except that the medium in which the light travels is not the fiber but free space (air). The transmitter (laser) and the photodetector (photodiode) are placed on building roof tops instead of burying fiber between the buildings. The major difference between fiber optic and free space optic communication is the attenuation. The attenuation in fiber is constant while the attenuation in free space (air) is dependent on weather conditions. Free Space optics can offer similar bit rates as fiber optics. Attenuation in FSO can be as good as fiber optics but it can also be extremely poor such that the link may be broken. More on this later.

The Solution (cont’d) High-speed Access (cont’d) Picture taken from: I. I. Kim, B. McArthur, and E. Korevaar, Comparison of laser beam propagation @ 785nm and 1550nm in fog and haze for optical wireless communications, Optical Access Incorporated, San Diego Since a fiber optic link can be replaced by a free space optic link, all other building can now connect to the fiber optic backbone through FSO providing bit rates from 100Mbps to 1.25Mbps. Here all buildings are connected in mesh configuration.

The Solution (cont’d) Typical FSO Laser/Photodiode Systems Photos taken from: http://www.systemsupportsolutions.com

FSO Limitations Power Link Budget Equation PTX – Power Transmitted PRX – Power Received dTX – Transmit Aperture Diameter (m) dRX – Receive Aperture Diameter (m) D – Beam Divergence (mrad) R – Range (km)  – atmospheric attenuation factor (dB/km)

FSO Limitations (cont’d) Atmospheric Attenuation Table taken from: I. I. Kim, and E. Korevaar, Availability of Free Space Optics (FSO) and hybrid FSO/RF systems, Optical Access Incorporated, San Diego Atmospheric attenuation is the most important factor determining the reliability of FSO. Attenuation is dependent on the weather conditions ( which is dependent on the city). Some Cities are very brutal for FSO (San Diego, CA) and some cities are excellent for FSO (Tuscan, AZ). This table shows the different attenuation numbers for different weather conditions and @ 2 wavelengths. Atmospheric Attenuation dependence on wavelength is very miniscule due to the logarithmic relation. There are other benefits for operating @ 1550nm instead of 785nm, which I will discuss in a bit. As

FSO Limitations (cont’d) TX/RX Alignment TX/RX Misalignment Unlike fiber optics, the precise alignment between the laser and the photodiode is another important factor for FSO. Here is a picture of laser spot at a very small distance away from the laser. However, as the laser moves through space the size of the spot grows! As it can bee seen here. For example, a 1.5mm laser spot diameter with a divergence angle of 1mrad, expands to 10.15cm @ a distance 100m away from the laser itself. And around 1km away the spot size can be around 1 – 5 meters. It can also be seen that first spot has its intensity confined in a smaller area than the second one. Obviously, the intensity at the center of the spot is always the highest and decreases as u move further away from the center. In this diagram, the amount of intensity/power being received from the laser beam is from the center. If there is any misalighnment, the power being received from the laser will not be from the center which will severely reduced the focused intensity. In this picture, a camera was mounted with the receiver to actually see the laser spot movements within the receiver sub-system. Picture taken from: TD. A. Rockwell, and G. S. Mecherle, Optical Wireless: Low-cost, Broadband, Optical Access, Fsona Communication Corporation, Richmond, BC

Limitation Solutions RF Back-up (Hybrid FSO/RF) Active Beam Tracking There are many alternative solutions out there to combat the unpredictable atmospheric attenuation and TX/RX misalignment issues. One is the use of a RF back up system in case the optical link goes down. These system are called Hybrid FSO/RF systems. Unfortunately, the RF backup does not provide bit rates anywhere near to what the optical link can offer. For misalignment issues, some manufacturers provide active beam tracking such that when the laser or the photodiode sub-systems begins to go out of alignment, one of the sub-systems adjusts its direction to compensate. Both of these solutions drive up the overall cost of the FSO system. Active Beam Tracking

Limitation Solutions (cont’d) Increase Laser Power Higher power received Higher power per unit area Operating @ 1550nm instead of 800nm Increase Average Power Efficiency (APE) Pulse Modulation Schemes can provide higher average power efficiency at the expense of higher BW requirement Hence, increase Peak-APE It is always desired to increase the power of any kind of transmitter to combat attenuation. However, there are always limitation in terms of how much power a laser can output. In terms of safety, any wavelength above 1400nm is absorbed by the lens and the cornea of our eyes. Hence, more power is allowed @ 1550nm. Even though PM schemes have a higher BW requirement, for OC there is enough BW to allow for this increase

Limitation Solutions (cont’d) On-Off Keying (OOK) Simplest solution based on intensity modulation ‘0’ – zero intensity, ‘1’ positive intensity Popular Pulse Time Modulation Schemes for OC Pulse Position Modulation (PPM) Pulse Interval Modulation (PIM)

Pulse Time Modulation PPM Higher average power efficiency than OOK Increases system complexity due to symbol-level synchronization. DPIM Higher APE than OOK but a bit lower than PPM No symbol-level synchronization required Higher Information capacity Data encoded as a number of time intervals between successive pulses Simplified receiver structure High Information Capacity means more bits can be added for error correction, etc.

Pulse Time Modulation (cont’d) Table taken from: A.R. Hayes, Z. Ghassemlooy, and N.L. See, The Effect of Baseline Wander on the Performance of Digital Pulse Interval Modulation, 1999 IEEE

Pulse Time Modulation (cont’d) M = log2L Picture Taken form: J. Zhang, Modulation Analysis for Outdoors Applications of Optical Wireless Communications, Nokia Networks Oy, Finland As you can see, less power is used for PPM and DPIM since the incoming data is stored in the time interval between 2 pulses. DPIM and PPM also use pulses with a much shorter pulse width. Hence, high power pulsed lasers (such as Q-Switched Lasers) can be used. Therefore, when higher power levels are being transmitted, this can help withstand the high attenuation. Plus any minor misalignment between the TX/RX would not be affect since the intensity of the laser beam away from the center will be higher than normal, hence increase the power received by the photodiode.

Pulse Time Modulation (cont’d) Bandwidth and Power Efficiency Comparisons Table Taken form: J. Zhang, Modulation Analysis for Outdoors Applications of Optical Wireless Communications, Nokia Networks Oy, Finland For M = 4, L = 16. For PPM BW = 4Rb. For DPIM BW = 2.375Rb,

Conclusion Power Increased by DPIM @ the cost of increased BW. Higher power means more power received @ the receiver @ high levels of attenuation and misalignment between TX/RX Major FSO benefit: reliable link connection and/or increased distance between TX/RX for certain cities