CORPORATE INSTITUTE OF SCIENCE & TECHNOLOGY , BHOPAL DEPARTMENT OF ELECTRONICS & COMMUNICATIONS MOSFET NOISE MODELS - Prof . Rakesh K . JHA.

Slides:



Advertisements
Similar presentations
Noise Lecture 6.
Advertisements

The Kinetic Theory of Gases
CHAPTER 4 CONDUCTION IN SEMICONDUCTORS
Chapter 3. Noise Husheng Li The University of Tennessee.
1 / 13 Fourier, bandwidth, filter. 2 / 13 The important roles of Fourier series and Fourier transforms: –To analysis and synthesis signals in frequency.
Integrated Circuits Laboratory Faculty of Engineering 29-April-2003 CMOS Noise Modeling For RF applications Presented by: Sameh Assem Ibrahim.
AME Int. Heat Trans. D. B. GoSlide 1 Non-Continuum Energy Transfer: Overview.
Lecture 6 Power spectral density (PSD)
Sep 22, 2005CS477: Analog and Digital Communications1 Random Processes and PSD Analog and Digital Communications Autumn
Low Noise Amplifier Design
Department of EECS University of California, Berkeley EECS 105 Fall 2003, Lecture 15 Lecture 15: Small Signal Modeling Prof. Niknejad.
Noise in BJT The objective is to determine, and for a bipolar transistor. The hybrid- model that includes the noise sources is shown below Fig 5-3 The.
Lecture 7: IC Resistors and Capacitors
Last Time Free electron model Density of states in 3D Fermi Surface Fermi-Dirac Distribution Function Debye Approximation.
Prof. ParkELC 2221 Lecture 1: Introductory Topics Prof. Park ELC 222 Essex County College.
1/f noise in devices 전광선.
4/11/2006BAE Application of photodiodes A brief overview.
Probability Theory and Random Processes
5. SOURCES OF ERRORS Noise types
1 Let g(t) be periodic; period = T o. Fundamental frequency = f o = 1/ T o Hz or  o = 2  / T o rad/sec. Harmonics =n f o, n =2,3 4,... Trigonometric.
Noise and Interference Any signal or phenomena which degrades signal to noise ratio (S/N). External 1.Thermal noise (raw or amplified) 2.On-channel unwanted.
Incoherent Scattering
© 2005 Pearson Prentice Hall This work is protected by United States copyright laws and is provided solely for the use of instructors in teaching their.
1 LECTURE 7. Contents 5.Sources of errors 5.1.Impedance matching Non-energetic matching Energetic matching Non-reflective matching To.
1/25 Noise in Analog CMOS ICs Gábor C. Temes School of Electrical Engineering and Computer Science Oregon State University March 2013.
1 In order to reduce errors, the measurement object and the measurement system should be matched not only in terms of output and input impedances, but.
Phase Noise and Oscillators Stephen Powell. What is an Oscillator?  Produces a signal at a particular frequency  They are everywhere! watches, radios,
ELEC 3105 Basic EM and Power Engineering Conductivity / Resistivity Current Flow Resistance Capacitance Boundary conditions.
PSD Chip Calculations. Energy Conversions Erad Energy of incident radiation (MeV) evis Energy of visible photon radiation (eV) εcon Conversion efficiency.
1 IEE5668 Noise and Fluctuations Prof. Ming-Jer Chen Dept. Electronics Engineering National Chiao-Tung University 03/11/2015 Lecture 3: Mathematics and.
Ya Bao, South Bank University 1 Noise Richard Read, The Essence of Communications Theory, Chapter 3.
Object of Plasma Physics
Statistical multipath channel models Hassan fayed DR.ENG MOHAB MANGOUD.
Electronics 1 Lecture 3 Moving Charge Carriers
Noise in SiGe HBT. outline Basic concepts and terminology about noise Representation of noise in bipolar by linear two- ports RF noise in bipolar –A unified.
NOISE IN COMMUNICATION CHANNELS
ارتباطات داده (883-40) فرآیندهای تصادفی نیمسال دوّم افشین همّت یار دانشکده مهندسی کامپیوتر 1.
COSC 4214: Digital Communications Instructor: Dr. Amir Asif Department of Computer Science and Engineering York University Handout # 3: Baseband Modulation.
2. Brownian Motion 1.Historical Background 2.Characteristic Scales Of Brownian Motion 3.Random Walk 4.Brownian Motion, Random Force And Friction: The Langevin.
Ludwid Boltzmann 1844 – 1906 Contributions to Kinetic theory of gases Electromagnetism Thermodynamics Work in kinetic theory led to the branch of.
教育部網路通訊人才培育先導型計畫 Probability, Random Processes and Noise 1 Outline 5.1 Probability Theory 5.2 Random Variables 5.3 Random Processes 5.4 Transmission of.
Electronic Noise Noise phenomena Device noise models
PIN DIODE CORPORATE INSTITUTE OF SCIENCE & TECHNOLOGY, BHOPAL DEPARTMENT OF ELECTRONICS & COMMUNICATIONS BY- PROF. RAKESH k. JHA.
Noise in Semiconductors
Lecture_02: Outline Thermal Emission
Review Of Statistical Mechanics Continued
Department of EECS University of California, Berkeley EECS 105 Fall 2003, Lecture 6 Lecture 6: Integrated Circuit Resistors Prof. Niknejad.
USSC2001 Energy Lecture 3 Thermodynamics of Heat Wayne M. Lawton Department of Mathematics National University of Singapore 2 Science Drive 2 Singapore.
C. Guazzoni – Advanced School and Workshop on Nuclear Physics Signal Processing - November 21, 2011 Noise mechanisms in electronic devices: physical origin.
1 Noise Analysis Electrical Noise Electrical noise is defined as any undesirable electrical energy. Figure 57 shows the effect of noise on an electrical.
What is thermal noise? Thermal noise in the resistance of the signal source is the fundamental limit on achievable signal sensitivity is unavoidable, and.
STATISTICAL MECHANICS PD Dr. Christian Holm PART 5-6 Some special topics, Thermal Radiation, and Plank distribution.
Application of photodiodes
ELEC 3105 Basic EM and Power Engineering
UNIT-III Signal Transmission through Linear Systems
Diffusion over potential barriers with colored noise
Development of a Pulse Shape Discrimination IC
SIGNALS PROCESSING AND ANALYSIS
Outline Introduction Signal, random variable, random process and spectra Analog modulation Analog to digital conversion Digital transmission through baseband.
Ideal Gases Kinetic Theory of Gases
Fundamentals of Heat Transfer
Noise Sources in Semiconductor Detectors
Lecture 13: Part I: MOS Small-Signal Models
Electronic Noise Noise phenomena Device noise models
Statistical Thermodynamics
Chapter 6 Random Processes
Ideal gas: Statistical mechanics
Chapter Three: Signals and Data Transmission
Fundamentals of Heat Transfer
CMOS FABRICATION PROCESSES
Presentation transcript:

CORPORATE INSTITUTE OF SCIENCE & TECHNOLOGY , BHOPAL DEPARTMENT OF ELECTRONICS & COMMUNICATIONS MOSFET NOISE MODELS - Prof . Rakesh K . JHA

MOSFET Noise

MOSFET Noise p.s.d. Saturation, strong inversion operation [A2/Hz] 1/f REGION WHITE NOISE REGION Saturation, strong inversion operation Where does factor g=2/3 come from?

Submicron CMOS: Noise behavior Gamma factor g > 2/3 ?!? Disagreement with long channel model? Question assumptions

Shot Noise Current noise density for DC current IDC Where does this come from? Key assumption: Electron arrivals independent events

Shot Noise What is current measured by ammeter?

Shot Noise What is current measured by ammeter?

Ramo-Shockley Theorem Current measured by ammeter: Randomly arriving pulses with area qe

Poisson Process AUTOCORRELATION Average arrival rate  [sec-1] Average DC current: Autocorrelation: time domain description of random process

Shot Noise Power Spectral Density Wiener-Khinchine theorem Autocorrelation  frequency domain p.s.d Frequency domain For frequencies < 1/T

Shot Noise Power Spectral Density Key Points: Discrete nature of charge is essential Carrier transits are independent events Carriers do not interact with each other or with any medium Temperature not a factor

Thermal Noise Current noise density for resistor Where does this come from? Assumption: Carriers in thermal equilibrium

Thermal Noise in Resistor Assumption: Carriers in thermal equilibrium Random velocity vectors v Only vx component contributes to current

"Temperature in this room is 293K" Boltzmann's Constant k k = 1.38 E-23 J/K Meaning? Thermodynamics: Equipartition theorem Independent energy storage modes in a system at equilibrium have average energy of kT/2 Equivalent statements: "Temperature in this room is 293K" "Average kinetic energy (in each of x, y, z directions) for each air molecule in this room is 2.02E-21 joule"

Thermal Noise Approximate collision statistics: Mean free path lc Mean free time tc 1 ps Velocity (rms) vx 0.1 µm/ps

Thermal Noise Consider "slice" equal to mean free path lc During one mean free time tc On average, half of carriers exit each way: IAVG+ = IAVG- Shot noise components is+ = -is- correlated Noise current from "slice" is = 2is+

Thermal Noise Sum (independent) contributions from slices Noise current seen by external ammeter im(s) reduced by current divider factor: DR of slice, total resistance R = R1 + DR + R2 Relating to R using mobility definition gives

Thermal Noise (Alternative) Equipartition, rms energy in capacitor: Integrate noise p.s.d. over noise bandwidth: Equate:

Thermal Noise Power Spectral Density Key Points: Discrete nature of charge is not essential Can also be derived from equipartition only (e.g. kT/C noise) Carrier scattering: interact with medium, thermal equilibrium Carrier transits are not independent due to interaction with medium Temperature is important to determine carrier average kinetic energy / velocity

Overview Creativity in Analog / Mixed Signal IC Design DSM CMOS Effects on Analog Design Fundamental Noise Sources Application MOSFET Noise Oscillator Jitter Conclusion

MOSFET Channel Noise Density Where does this come from? Assumption: Resistive channel segments

THE END