UNIT III. By Ajay Kumar Gautam Asst. Prof. Electronics & Communication Engineering Dev Bhoomi Institute of Technology & Engineering, Dehradun

Similar documents
Optical Receivers Theory and Operation

Photodiode: LECTURE-5

Avalanche Photodiode. Instructor: Prof. Dietmar Knipp Presentation by Peter Egyinam. 4/19/2005 Photonics and Optical communicaton

OFCS OPTICAL DETECTORS 11/9/2014 LECTURES 1

Lecture 18: Photodetectors

Optical Fiber Communication Lecture 11 Detectors

Detectors for Optical Communications

Chap14. Photodiode Detectors

FIBER OPTICS. Prof. R.K. Shevgaonkar. Department of Electrical Engineering. Indian Institute of Technology, Bombay. Lecture: 20

OPTOELECTRONIC and PHOTOVOLTAIC DEVICES

Lecture 9 External Modulators and Detectors

Optical Amplifiers. Continued. Photonic Network By Dr. M H Zaidi

Comparative Study of an Optical Link with PIN and APD as Photo-Detector Preetam Jain 1, Dr Lochan Jolly 2

Key Questions ECE 340 Lecture 28 : Photodiodes

Chapter 3 OPTICAL SOURCES AND DETECTORS

LEDs, Photodetectors and Solar Cells

MAHALAKSHMI ENGINEERING COLLEGE TIRUCHIRAPALLI

Problem 4 Consider a GaAs p-n + junction LED with the following parameters at 300 K: Electron diusion coecient, D n = 25 cm 2 =s Hole diusion coecient

UNIT-III SOURCES AND DETECTORS. According to the shape of the band gap as a function of the momentum, semiconductors are classified as

Lecture 7:PN Junction. Structure, Depletion region, Different bias Conditions, IV characteristics, Examples

Lecture 14: Photodiodes

Optical Communications

Physics of Waveguide Photodetectors with Integrated Amplification

Solar Cell Parameters and Equivalent Circuit

OPTI510R: Photonics. Khanh Kieu College of Optical Sciences, University of Arizona Meinel building R.626

Figure Responsivity (A/W) Figure E E-09.

LED lecture. Wei Chih Wang University of Washington

Figure Figure E E-09. Dark Current (A) 1.

Recent Development and Study of Silicon Solid State Photomultiplier (MRS Avalanche Photodetector)

Fundamentals of CMOS Image Sensors

CHAPTER 8 The PN Junction Diode

Optical Sources and Detectors

SUPPLEMENTARY INFORMATION

CMOS Phototransistors for Deep Penetrating Light

Investigate the characteristics of PIN Photodiodes and understand the usage of the Lightwave Analyzer component.

What is the highest efficiency Solar Cell?

Opto-electronic Receivers

10/14/2009. Semiconductor basics pn junction Solar cell operation Design of silicon solar cell

10/27/2009 Reading: Chapter 10 of Hambley Basic Device Physics Handout (optional)

Analysis and Optimization of PIN photodetectors for optical communication Cláudio Miguel Caramona Fernandes

SYLLABUS Optical Fiber Communication

Photon Count. for Brainies.

An Introduction to the Silicon Photomultiplier

UNIT - 5 OPTICAL RECEIVER

Optical Sources & Detectors for Fiber Optic communication

1 Semiconductor-Photon Interaction

Photons and solid state detection

PHYSICAL ELECTRONICS(ECE3540) APPLICATIONS OF PHYSICAL ELECTRONICS PART I

Electronic devices-i. Difference between conductors, insulators and semiconductors

A silicon avalanche photodetector fabricated with standard CMOS technology with over 1 THz gain-bandwidth product

CONTENTS. 2.2 Schrodinger's Wave Equation 31. PART I Semiconductor Material Properties. 2.3 Applications of Schrodinger's Wave Equation 34

Design and Simulation of N-Substrate Reverse Type Ingaasp/Inp Avalanche Photodiode

UNIT VIII-SPECIAL PURPOSE ELECTRONIC DEVICES. 1. Explain tunnel Diode operation with the help of energy band diagrams.

New Silicon Reach-Through Avalanche Photodiodes with Enhanced Sensitivity in the DUV/UV Wavelength Range

Mechatronics and Measurement. Lecturer:Dung-An Wang Lecture 2

ECE 340 Lecture 29 : LEDs and Lasers Class Outline:

Key Questions. What is an LED and how does it work? How does a laser work? How does a semiconductor laser work? ECE 340 Lecture 29 : LEDs and Lasers

Study and Measurement of the Main Parameters of a Laser quadrant Detector

Ultra-sensitive SiGe Bipolar Phototransistors for Optical Interconnects

14.2 Photodiodes 411

for optical communication system

CHAPTER 8 The PN Junction Diode

Optical Fibre Communication Systems

Department of Electrical Engineering IIT Madras

Review of Semiconductor Physics

MOSFET short channel effects

Performance and Characteristics of Silicon Avalanche Photodetectors in

Development of High Sensitivity SWIR APD Receivers

Silicon Avalanche Photodetectors Fabricated With Standard CMOS/BiCMOS Technology Myung-Jae Lee

LAB V. LIGHT EMITTING DIODES

Detectors for microscopy - CCDs, APDs and PMTs. Antonia Göhler. Nov 2014

Chapter 2 PN junction and diodes

Examination Optoelectronic Communication Technology. April 11, Name: Student ID number: OCT1 1: OCT 2: OCT 3: OCT 4: Total: Grade:

A Thesis submitted in partial fulfillment of the requirements for the degree of Master of Science at George Mason University

ECEN 4606, UNDERGRADUATE OPTICS LAB

Light Sources, Modulation, Transmitters and Receivers

Lecture 4 Fiber Optical Communication Lecture 4, Slide 1

SSRG International Journal of Medical Science (SSRG-IJMS) volume1 issue1 August 2014

Characterisation of SiPM Index :

Semiconductor Devices Lecture 5, pn-junction Diode

Engineering Medical Optics BME136/251 Winter 2018

Prepared by: Dr. Rishi Prakash, Dept of Electronics and Communication Engineering Page 1 of 5

Frequency Dependent Harmonic Powers in a Modified Uni-Traveling Carrier (MUTC) Photodetector

Lecture 8 Optical Sensing. ECE 5900/6900 Fundamentals of Sensor Design

High-speed Ge photodetector monolithically integrated with large cross silicon-on-insulator waveguide

Modulation of light. Direct modulation of sources Electro-absorption (EA) modulators

Lecture 9: Limiting and Clamping Diode Circuits. Voltage Doubler. Special Diode Types.

Lecture 24: Bipolar Junction Transistors (1) Bipolar Junction Structure, Operating Regions, Biasing

Optodevice Data Book ODE I. Rev.9 Mar Opnext Japan, Inc.

Bipolar Junction Transistor (BJT)

Downloaded from

CHAPTER 8 The pn Junction Diode

SRM UNIVERSITY FACULTY OF ENGINEERING AND TECHNOLOGY SCHOOL OF ELECTRONICS AND ELECTRICAL ENGINEERING DEPARTMENT OF TCE COURSE PLAN

NON-AMPLIFIED PHOTODETECTOR USER S GUIDE

Luminous Equivalent of Radiation

ELEC 3908, Physical Electronics, Lecture 16. Bipolar Transistor Operation

Unit 2 Semiconductor Devices. Lecture_2.5 Opto-Electronic Devices

FIBER OPTICS. Prof. R.K. Shevgaonkar. Department of Electrical Engineering. Indian Institute of Technology, Bombay. Lecture: 18.

Electronics I. Midterm #1

Exp 3 COLCULATE THE RESPONSE TIME FOR THE SILICON DETECTOR

Transcription:

UNIT III By Ajay Kumar Gautam Asst. Prof. Electronics & Communication Engineering Dev Bhoomi Institute of Technology & Engineering, Dehradun

SYLLABUS Optical Absorption in semiconductors, Types of Photo Diodes, Principle of photo detection, working and structures of p-i-n and APD photo detectors, noises in photo detectors, SNR, detector response time effects, comparison of various photo detectors. September 6, 2013 By: Ajay Kumar Gautam, DBITW, Dehradun 1

LECTURE PLAN UNIT-III OPTICAL DETECTORS Optical Absorption in semiconductors 2/329-332 Types of Photo Diodes, Principle of photo detection 2/328-329 Working and structures of p-i-n and APD photo detectors 1/223-230 noises in photo detectors, SNR 1/231-234 detector response time effects 1/235-239 comparison of various photo detectors 1/244 September 6, 2013 By: Ajay Kumar Gautam, DBITW, Dehradun 2

Introduction In case of any communication, there must be a device which can receive the transmitted signal. In case of OFC system, the first element of the receive is a photodetector. Photodetectors are semiconductor devices that can convert optical signals into electrical signals. September 6, 2013 By: Ajay Kumar Gautam, DBITW, Dehradun 3

Cond... The function of the photodector is to: sense the optical light convert it into electrical variations. Hence referred O/E Converter. Since the optical signal is very weak and distorted signal, so the photodetector must be able to sense the weak signals & it must be high performance device. September 6, 2013 By: Ajay Kumar Gautam, DBITW, Dehradun 4

Basic Requirement for the Photodetectors 1. Good Sensitivity: it must be able to produce maximum electrical signal for a given amount of optical power, i.e., the quantum efficiency should be high. 2. Fast Response Time: to obtain higher bandwidth 3. Compatible Physical Dimensions: Small Size for efficient coupling to the fiber. 4. Highly Stable: the performance characteristic of the detector must be independent of the ambient conditions. 5. High Reliability: so that it can perform its function for a long time continuously. 6. Low Biasing Voltages or Current: should not require excessive bias voltage or current. September 6, 2013 By: Ajay Kumar Gautam, DBITW, Dehradun 5

PHYSICAL PRINCIPLE OF PHOTODIODE September 6, 2013 By: Ajay Kumar Gautam, DBITW, Dehradun 6

PIN Photodector The pin refers to positive intrinsic negative. September 6, 2013 By: Ajay Kumar Gautam, DBITW, Dehradun 7

Cond So, the device consists of 3 layers. P and N regions are separated by very lightly n-doped intrinsic (i) region. The reverse bias voltage is applied across the device, so that the i region is fully depleted of carriers. September 6, 2013 By: Ajay Kumar Gautam, DBITW, Dehradun 8

Cond... Now, the photon can give its energy and excite an electron from the valance band to the conduction band, only when the incident photon has an energy greater than or equal to the band gap energy of this semiconductor material. September 6, 2013 By: Ajay Kumar Gautam, DBITW, Dehradun 9

Cond... This process will generates mobile electron-hole pairs as shown on next slide. These electrons and holes are known photocarriers, since they are photogenerated charge carriers. September 6, 2013 By: Ajay Kumar Gautam, DBITW, Dehradun 10

September 6, 2013 By: Ajay Kumar Gautam, DBITW, Dehradun 11

Cond... These charge carriers are available to produce a current flow, when a bias voltage is applied across the device. The most of the incident light is absorbed in the depletion region, so the photocarriers are generated in this depletion region. September 6, 2013 By: Ajay Kumar Gautam, DBITW, Dehradun 12

Cond... A high electric field is available in the depletion region, so it will cause the carriers to separate. These carriers are collected across the reverse bias junction. The current will flow because of these carriers. The one electron will flow for every carrier pair generated. This current is known as photocurrent. September 6, 2013 By: Ajay Kumar Gautam, DBITW, Dehradun 13

Cond... Since the charge carriers flow through the material, the electron-hole pair will recombine and hence disappear. On average, the charge carriers move a distance L n or L p for electrons and holes respectively. September 6, 2013 By: Ajay Kumar Gautam, DBITW, Dehradun 14

Cond... This distance is known as the diffusion length. The time for recombination or electron or hole is known as carrier lifetime. The lifetime and the diffusion lengths are related by: Ln Dn n & Lp Dp p September 6, 2013 By: Ajay Kumar Gautam, DBITW, Dehradun 15

Cond... L & L Diffusionlength for elctrons & holes respectively n & n p p Carrier Lifetime for elctrons & holes respectively D & D Diffusion coeffient for elctrons & holes respectively n p As a photon flux Φ penetrates into a semiconductor, it will be absorbed as it progresses through the material. September 6, 2013 By: Ajay Kumar Gautam, DBITW, Dehradun 16

Cond... Let, Pin is the optical power level, that falls on the photodector at x = 0 and P(x) is the power level at distance x into the material. The incremental distance dx in the semiconductor is given by: dp( x) ( ) P( x) dx s September 6, 2013 By: Ajay Kumar Gautam, DBITW, Dehradun 17

Cond... Integrating this relation gives, P x s ( ) x ( ) Pine s is photon absorption coefficient The upper wavelength cutoff is determined by band-gap energy E g of the material. September 6, 2013 By: Ajay Kumar Gautam, DBITW, Dehradun 18

Cond... hc 1.24 c ( m) E ( ev ) E ( ev ) g The photocurrent I P produced by incident light of optical power P o is given by: q I p Pin (1 sw)(1 Rf ) h g September 6, 2013 By: Ajay Kumar Gautam, DBITW, Dehradun 19

Cond... Where, R f is reflectivity at the entrance of the photodiode P in is the optical incident power q is the electron charge hv is the photon energy September 6, 2013 By: Ajay Kumar Gautam, DBITW, Dehradun 20

Cond... Photodector have two quantum efficiency and its response speed. These parameters depend on the material band gap, the operating wavelength, and the doping and thickness of the, p, i, and n regions of the device. September 6, 2013 By: Ajay Kumar Gautam, DBITW, Dehradun 21

Cond... The quantum efficiency is the no of electron-hole carrier pair generated per incident is given by: no of electron hole pair generated Ip / q no of incident photons P / h I q p R P in h in September 6, 2013 By: Ajay Kumar Gautam, DBITW, Dehradun 22

Cond... R is the responsivity of the photodiode. The photocurrent (I p ) is directly proportional to the incident optical power (P in ). Quantum efficiency varies according to the photon energy. September 6, 2013 By: Ajay Kumar Gautam, DBITW, Dehradun 23

Avalanche Photodiodes September 6, 2013 By: Ajay Kumar Gautam, DBITW, Dehradun 24

Problems: Example 6.1, 2, 3 4, 6 & 7 from Keiser. September 6, 2013 By: Ajay Kumar Gautam, DBITW, Dehradun 25

Review Problems How is silicon RAPD operated? How does it differ from p-i-n photodiode? What are the advantages and disadvantages?[uptu 2009-10] Define quantum efficiency and responsivity of a photo-detector. Calculate the transit time for silicon photodiode which has a saturation of 10 5 ms -1. The depletion layer thickness is 7 µm. [UPTU 2009-10] Explain the requirements of optical detector to be used for the purpose of optical communication. What are the parameters by which performance of optical detector can be judged?[uptu 2010-11] September 6, 2013 By: Ajay Kumar Gautam, DBITW, Dehradun 26

Review Problems Describe the working and principle of pin photodiode. How its efficiency can be increased. [UPTU 2010-11] Write short notes [UPTU 2010-11] RAPD photo-detector Noise sources in optical fiber communication. What is the significance of intrinsic layer in PIN diode? What is the principle of working of PIN diode [UPTU 2011-12] Define quantum efficiency and responsivity of a photodiode. Determine the wavelength at which quantum efficiency and responsivity are equal [UTU 2011-12] September 6, 2013 By: Ajay Kumar Gautam, DBITW, Dehradun 27

Review Problems Discuss the working principle of avalanche photodiode, how it differs from p-i-n photodiode? State the advantages and drawbacks with the use of the RAPD as a detector for optical fiber communications. [UTU 2011-12] Explain the physical principle of APD. What is the temperature effect on Avalanche Gain? Describe Automatic Gain Control using Op-amp. [UPTU 2011-12] Explain the working of a P-I-N photodiode. Also explain the factors that limit the speed of response of photodiode [UTU 2012-13] Explain the impact ionization in avalanche photodiodes. Define photo multiplication factor and cutoff over length of photodiode. [UTU 2012-13] September 6, 2013 By: Ajay Kumar Gautam, DBITW, Dehradun 28

Review Problems Discuss the expression for the SNR in an APD receiver. How the signal to noise ratio may be modified to give the optimum avalanche multiplication factor [UTU 2012-13] Describe surface LED and PIN photodiode always operative in reverse bias region. [UTU 2012-13] September 6, 2013 By: Ajay Kumar Gautam, DBITW, Dehradun 29

REFRENCES 1. Optical Fiber Communications Gerd Keiser, Mc Graw-Hill International edition, 4 TH Edition, 2008. 2. Optical Fiber Communications John M. Senior, PHI, 2 nd Edition, 2002. 3. Optical Fiber Communications Gerd Keiser, Mc Graw-Hill International edition, 2 ND Edition, 2000. 4. Fiber Optic Communication Systems Govind P. Agarwal, John Wiley, 3 rd Edition, 2004 5. Text Book on Optical Fibre Communication and its Applications S. C. Gupta, PHI, 2005. 6. Fiber Optic Communications D.K. Mynbaev, S.C. Gupta and Lowell L. Scheiner, Pearson Education, 2005 7. Optical Communication System- R. K. Singh, Wiley India, Delhi September 6, 2013 By: Ajay Kumar Gautam, DBITW, Dehradun 30