Lecture Frequency Synthesizers - I (6/25/03) Page 170-1

Similar documents
LECTURE 1 CMOS PHASE LOCKED LOOPS

Chapter 2 Introduction: From Phase-Locked Loop to Costas Loop

Receiver Architectures

UNIT IV DIGITAL MODULATION SCHEME

Solution of ECE 342 Test 2 S12

Chapter 2 Summary: Continuous-Wave Modulation. Belkacem Derras

Communication Systems. Department of Electronics and Electrical Engineering

Communications II Lecture 7: Performance of digital modulation

f t 2cos 2 Modulator Figure 21: DSB-SC modulation.

Signal Characteristics

Analog/Digital Communications Primer

Passband Data Transmission I References Phase-shift keying Chapter , S. Haykin, Communication Systems, Wiley. G.1

Wrap Up. Fourier Transform Sampling, Modulation, Filtering Noise and the Digital Abstraction Binary signaling model and Shannon Capacity

Principles of Communications

Chapter 4: Angle Modulation

Chapter 4: Angle Modulation

FROM ANALOG TO DIGITAL

ANALOG AND DIGITAL SIGNAL PROCESSING LABORATORY EXPERIMENTS : CHAPTER 3

Optical Short Pulse Generation and Measurement Based on Fiber Polarization Effects

ECE ANALOG COMMUNICATIONS - INVESTIGATION 7 INTRODUCTION TO AMPLITUDE MODULATION - PART II

TELE4652 Mobile and Satellite Communications

Passband Data Transmission II References Frequency-shift keying Chapter 6.5, S. Haykin, Communication Systems, Wiley. H.1

Communication Systems. Communication Systems

ECMA st Edition / June Near Field Communication Wired Interface (NFC-WI)

An Open-Loop Class-D Audio Amplifier with Increased Low-Distortion Output Power and PVT-Insensitive EMI Reduction

Memorandum on Impulse Winding Tester

Lecture 5: DC-DC Conversion

Synchronization of single-channel stepper motor drivers reduces noise and interference

Analog Circuits EC / EE / IN. For

Test 1 Review. Test 1 Review. Communication Systems: Foundational Theories. Communication System. Reference: Sections and

EXPERIMENT #4 AM MODULATOR AND POWER AMPLIFIER

Investigation and Simulation Model Results of High Density Wireless Power Harvesting and Transfer Method

EE201 Circuit Theory I Fall

Modulation exercises. Chapter 3

EXPERIMENT #9 FIBER OPTIC COMMUNICATIONS LINK

High Gain Opamp based Comparator Design for Sigma Delta Modulator

Active Filters - 1. Active Filters - 2

P. Bruschi: Project guidelines PSM Project guidelines.

ECMA-373. Near Field Communication Wired Interface (NFC-WI) 2 nd Edition / June Reference number ECMA-123:2009

Table of Contents. 3.0 SMPS Topologies. For Further Research. 3.1 Basic Components. 3.2 Buck (Step Down) 3.3 Boost (Step Up) 3.4 Inverter (Buck/Boost)

Industrial, High Repetition Rate Picosecond Laser

EE 330 Lecture 24. Amplification with Transistor Circuits Small Signal Modelling

Noise Reduction/Mode Isolation with Adaptive Down Conversion (ADC)

EE 40 Final Project Basic Circuit

Digital Communications - Overview

Synchronization of the bit-clock in the receiver

Problem Sheet: Communication Channels Communication Systems

EE558 - Digital Communications

4 20mA Interface-IC AM462 for industrial µ-processor applications

M2 3 Introduction to Switching Regulators. 1. What is a switching power supply? 2. What types of switchers are available?

4.5 Biasing in BJT Amplifier Circuits

ECE3204 Microelectronics II Bitar / McNeill. ECE 3204 / Term D-2017 Problem Set 7

Software solutions to mitigate the EM emission of power modules

Generating Polar Modulation with R&S SMU200A

Communications II Lecture 5: Effects of Noise on FM. Professor Kin K. Leung EEE and Computing Departments Imperial College London Copyright reserved

Pulse Train Controlled PCCM Buck-Boost Converter Ming Qina, Fangfang Lib

Obsolete Product(s) - Obsolete Product(s)

Lecture 4. EITN Chapter 12, 13 Modulation and diversity. Antenna noise is usually given as a noise temperature!

Research Article AD-PLL for WiMAX with Digitally-Regulated TDC and Glitch Correction Logic

Notes on the Fourier Transform

ISSCC 2007 / SESSION 29 / ANALOG AND POWER MANAGEMENT TECHNIQUES / 29.8

Jitter Analysis of Current-Mode Logic Frequency Dividers

Diodes. Diodes, Page 1

A WIDEBAND RADIO CHANNEL MODEL FOR SIMULATION OF CHAOTIC COMMUNICATION SYSTEMS

unmodulated carrier phase refference /2 /2 3π/2 APSK /2 3/2 DPSK t/t s

An Improved Zero-Voltage-Transition Technique in a Single-Phase Active Power Factor Correction Circuit

ESD. What is ESD? Lightning to the buildings. ESD to IC s. ESD protection circuit for IC s. Lightning Rod for Buildings

Folded Multiple-Capture: An Architecture for High Dynamic Range Disturbance-Tolerant Focal Plane Array

Question 1 TELE4353. Average Delay Spread. RMS Delay Spread = = Channel response (2) Channel response (1)

Revision: June 11, E Main Suite D Pullman, WA (509) Voice and Fax

ORDER INFORMATION TO pin 320 ~ 340mV AMC7150DLF

Power losses in pulsed voltage source inverters/rectifiers with sinusoidal currents

Chapter 14: Bandpass Digital Transmission. A. Bruce Carlson Paul B. Crilly 2010 The McGraw-Hill Companies

13.1 Analog/Digital Lowpass Butterworth Filter


Technology Trends & Issues in High-Speed Digital Systems

Accurate Tunable-Gain 1/x Circuit Using Capacitor Charging Scheme

RITEC, Inc. 60 Alhambra Rd., Suite 5 Warwick, RI (401) FAX (401) Powerful Ultrasonic Research Tool. A Modular Approach

Phase-Shifting Control of Double Pulse in Harmonic Elimination Wei Peng1, a*, Junhong Zhang1, Jianxin gao1, b, Guangyi Li1, c

Sensing, Computing, Actuating

Analog Baseband Communication Systems. Digital Baseband Communication Systems

Double Edge Class BD Hybrid DPWM Implementation Using Linearized LBDD Algorithm

PLL Hardware Design and Software Simulation using the 32-bit version of SystemView by ELANIX Stephen Kratzet, ELANIX, Inc.

MX629. DELTA MODULATION CODEC meets Mil-Std DATA BULLETIN. Military Communications Multiplexers, Switches, & Phones

Lecture 11. Digital Transmission Fundamentals

Optical phase locked loop for transparent inter-satellite communications

Chapter 1: Introduction

Microwave Transistor Oscillator Design

Lecture #7: Discrete-time Signals and Sampling

Dimensions. Transmitter Receiver ø2.6. Electrical connection. Transmitter +UB 0 V. Emitter selection. = Light on = Dark on

6.776 High Speed Communication Circuits Lecture 17 Noise in Voltage Controlled Oscillators

ECS455: Chapter 4 Multiple Access

The Delay-Locked Loop

Dimensions. Transmitter Receiver ø2.6. Electrical connection. Transmitter +UB 0 V. Emitter selection. = Light on = Dark on

Dimensions. Model Number. Electrical connection emitter. Features. Electrical connection receiver. Product information. Indicators/operating means

3. Carrier Modulation Analog

Pointwise Image Operations

Chapter 2: Fourier Representation of Signals and Systems

READING ASSIGNMENTS LECTURE OBJECTIVES. Problem Solving Skills. x(t) = cos(αt 2 ) ELEG-212 Signal Processing and Communications

Development of Temporary Ground Wire Detection Device

Transcription:

Lecure 170 Frequency Synhesizers I (6/25/03) Page 1701 LECTURE 170 APPLICATIONS OF PLLS AN FREQUENCY IVIERS (PRESCALERS) (References [2, 3, 4, 6, 11]) Objecive The objecive of his presenaion is: 1.) Examine he applicaions of PLLs 2.) evelop and characerize he echniques used for frequency division Ouline Applicaions of PLLs Inegraed Circui Frequency Synhesizers Archiecures and Techniques ividers for Frequency Synhesizers NoiseShaping Techniques Summary Lecure 170 Frequency Synhesizers I (6/25/03) Page 1702 APPLICATIONS OF PLLS The PLL The PLL is a very versaile building block and is suiable for a variey of applicaions including: 1.) emodulaion and modulaion 2.) Signal condiioning 3.) Frequency synhesis 4.) Clock and daa recovery 5.) Frequency ranslaion

Lecure 170 Frequency Synhesizers I (6/25/03) Page 1703 FM emodulaion When he PLL is locked on a frequency modulaed signal, he conrolling volage o he VCO becomes proporional o he frequency. v in Phase eecor Loop Filer Posdeecion Filer v ou VCO v c v in f 1 f 2 f 1 V 2 v ou V 1 Fig. 4.101 Can be used for frequency shif keying (FSK) if a volage discriminaor is placed a he oupu. Lecure 170 Frequency Synhesizers I (6/25/03) Page 1704 FM emodulaion Example If K o = 2π(1kHz/Vol), K v = 500 (sec1) and ω o = 1000π rads/sec ( = 500Hz) for he FM demodulaor on he previous slide, (a.) Find V o for f i = 250Hz and 1000Hz. (b.) Wha is he ime consan of V o for a sep change beween hese wo frequencies? Soluion (a.) We know ha ω i ω o ω osc = ω i = ω o K o V o V o = K o V o (250Hz) = 250500 1000 = 0.25V V o (1000Hz) = 1000500 1000 = 0.5V (b.) τ = 1 K v = 2ms We noe ha he riseimes of he square wave on he previous page would no longer be zero bu ake abou 10ms o go from one level o anoher.

Lecure 170 Frequency Synhesizers I (6/25/03) Page 1705 FM emodulaor Example Coninued Example: For he PLL of he previous example, find v o () if he inpu signal is frequency modulaed so ha ω i () = 2π(500Hz)[10.1sin(2πx102)]. Soluion V o (jω) ω i (jω) = 1 K v K o K v jω = 1 K v K o K v j2πx100 ω=200π 1 500 = 2000π 500j628 = 1 2000π (0.39j0.48) ω i (jω) = 0.1(1000π) = 100π = 50(2π) V o (jω) = 50 50 1000 (0.39j0.48) = 1000 0.62/51 = 0.031/51 or v o () = 0.031 sin[(2πx102)51 ] Lecure 170 Frequency Synhesizers I (6/25/03) Page 1706 Phase Modulaor When he PLL is locked on a fixed frequency, a slowly varying signal, v m (), can be used o cause he phase shif he VCO o shif achieving a phase modulaor. Phase modulaion signal v m () Phase eecor Loop Filer vc VCO v ou Fig. 4.1025 v ou () = V ou cos[ω ref θ m ()] where θ m () = 1 K d v m()

Lecure 170 Frequency Synhesizers I (6/25/03) Page 1707 Signal Condiioning The PLL can operae as a narrowband filer wih an exremely high Q o selec a desired signal in he presence of undesired signals. v in Phase eecor Loop Filer v c VCO v ou ω c ω c Fig. 4.102 This applicaion represens a radeoff in he capure range and he loop bandwidh. If he loop bandwidh is small, he SNR of he oupu can be much greaer han he inpu. If he loop bandwidh is large, he capure range for he desired signal is larger (can rack he desired signal beer). Lecure 170 Frequency Synhesizers I (6/25/03) Page 1708 Frequency Synhesis ividers placed in he feedback and/or inpu allow he generaion of frequencies based on a sable reference frequency. M Volage which makes f = LO M N M Phase eecor Loop Filer VCO u = M N f LO N N Oscillaor conrol volage Fig. 4.103A When he phase deecor is locked, he wo incoming frequencies are equal. Therefore, M = u N u = N M

Lecure 170 Frequency Synhesizers I (6/25/03) Page 1709 Clock and aa Recovery The funcion of a clock and daa recovery circui is o produce a sable iming signal from a sream of binary daa. Clock recovery consiss of wo basic funcions: 1.) Edge deecion 2.) Generaion of a sable periodic oupu in Edge eecor Phase eecor Loop Filer v c VCO Clock Fig. 4.104 Lecure 170 Frequency Synhesizers I (6/25/03) Page 17010 Jier Suppression In digial communicaions, ransmier or rerieved daa may suffer from iming jier. A PLL clock recovery circui can be used o regenerae he signal and eliminae he jier as shown below. Flipflop in Q ou Clock Recovery Circui in Clock ou Fig. 4.105

Lecure 170 Frequency Synhesizers I (6/25/03) Page 17011 Frequency Translaion The PLL can be used o ranslae he frequency of a highly sable bu fixed frequency oscillaor by a small amoun in frequency. Someimes called frequency offse loop. sc ± fosc f 1 Mixer LPF Phase eecor Loop Filer vc VCO u = f 1 sc Fig. 4.106 Lecure 170 Frequency Synhesizers I (6/25/03) Page 17012 IC FREQUENCY SYNTHESIZERS ARCHITECTURES AN TECHNIQUES Synhesizer Specificaions for Various Wireless Sandards Wireless Sandard Frequency Range (MHz) Channel Spacing Number of Channels Swiching Time GSM Rx: 935960 200kHz 124 800µs Tx: 890915 CS1800 Rx: 18051880 200kHz 374 800µs Tx: 17101785 PCS1900 Rx: 19301990 200kHz 800µs Tx: 17101785 ECT 18801900 1.728MHz 10 450µs AMPS Rx: 869894 30kHz 832 Slow Tx: 824849 CMA Rx: 869894 1.25MHz 20 Tx: 824849 PHS1900 Rx: 18951918 300kHz 300 1.5ms IS54 Rx: 869894 30kHz 832 Slow Tx: 824849 WLAN 24002483 1MHz 79 Several µs

Lecure 170 Frequency Synhesizers I (6/25/03) Page 17013 Componens of a Frequency Synhesizer Funcion of a frequency synhesizer is o generae a frequency from a reference frequency. Block diagram: Reference Frequency Phase Frequency eecor (PF) LPF VCO Componens: Phase/frequency deecor oupus a /N ivider (1/N) Fig. 12.416 signal ha is proporional o he difference beween he frequency/phase of wo inpu periodic signals. The lowpass filer is use o reduce he phase noise and enhance he specral puriy of he oupu. The volageconrolled oscillaor akes he filered oupu of he PF and generaes an oupu frequency which is conrolled by he applied volage. The divider scales he oupu frequency by a facor of N. = N = N Lecure 170 Frequency Synhesizers I (6/25/03) Page 17014 Basic Frequency Synhesizer Archiecure Simple frequency synhesizer: Reference Frequency Phase Frequency eecor (PF) LPF VCO /N ivider (1/N) Fig. 12.416 Commens: Frequency sep size is equal o. Thus, for small channel spacing,, is small which makes N large. Large N resuls in an increase in he inband phase noise of he VCO signal by 20log(N). = N

Lecure 170 Frequency Synhesizers I (6/25/03) Page 17015 Basic Frequency Synhesizer Archiecure Coninued Frequency Synhesizer wih a SingleModulus Prescaler: PF LPF VCO Programmable ivider 1/N p Commens: = N P P Only he prescaler needs o run a very high speed Prescaler 1/P Fig. 12.417 Since P is fixed, he value of N P is smaller causing increased channel spacing resuls in increased lockon ime and sidebands a undesirable frequencies Soluion: 1/P /P PF LPF VCO Programmable ivider 1/N p Prescaler 1/P Fig. 12.418 Lecure 170 Frequency Synhesizers I (6/25/03) Page 17016 Basic Frequency Synhesizer Archiecure Coninued Frequency Synhesizer wih a ualmodulus Prescaler: Operaion: 1.) The modulus conrol signal is low a he beginning of a coun cycle enabling he prescaler o divide by P 1 unil he A couner couns o zero. 2.) The modulus conrol signal goes high enabling he prescaler o divide by P, unil he N P couner couns down he res of he way o zero (N P A). 3.) Thus, N = (N P A)P A(P1) = N P A = (N P A). 4.) The modulus conrol is se back low, he couners are rese o heir respecive programmed values and he sequence is repeaed. Commens: N P > A The value of P divided by he maximum frequency of he VCO mus no exceed he frequency capabiliy of he N P and A couners. P imes he period of he maximum VCO frequency > he sum of he propagaion delay hrough he dualmodulus prescaler plus he prescaler seup or release ime relaive o is conrol signal plus he propagaion delay of o he modulus conrol. PLL N P Couner ualmodulus 1/N Prescaler P 1/P or 1/(P1) A Couner Conrol Logic Fig. 12.419

Lecure 170 Frequency Synhesizers I (6/25/03) Page 17017 Example ual Modulus Frequency Synhesizer A block diagram for a dual modulus frequency synhesizer is shown. (a.) If his synhesizer divides he VCO oupu by N1 every K VCO cycles and by N for he res of he ime, express he oupu frequency, u, as a funcion of N, K, and. (b.) If you waned o use his frequency synhesizer o generae an oupu frequency of 27.135MHz from a reference frequency of 100kHz, wha would be he value of N and how many cycles ou of 100 would you divide by N1 where he remaining cycles you would divide by N? Soluion (a.) The average divide facor is expressed as N eff = (N1)xuy cycle for N1 Nxuy cycle for N PLL N,N1 Modulus Conrol u F00FE01 1 = (N1) K N 1 1 K = N1 K f ou = N eff = N 1 K f ref (b.) ividing 27.135MHz by 100kHz gives 271.35. Therefore, choose N = 271 and divide by N1 or 272 for 35 cycles ou of 100 and by N for he remaining 65 cycles. Thus, N = 271 and K = 35 cycles for every 100 cycles Lecure 170 Frequency Synhesizers I (6/25/03) Page 17018 FracionalN Frequency Synhesizer The oupu frequency can be finer han because division raio in he feedback loop does no have o be an ineger. Operaion: Make he division raio alernae beween N or N 1 in a conrolled and repeiive fashion o average an inermediae value beween N and N 1. For example, assume ha he synhesizer divides by N 1 every L cycles and by N he res of he ime. The average division raion is N aver = N 1 L. Therefore, 1 = (N1) L N 1 1 L f ref = N 1 L f ref FracionalN Techniques: Technique Feaure Problem AC phase esimaion Cancel spurs by AC Analog mismach Random Jiering Randomize divider Frequency jier Σ modulaion Modulae he divider raio Quanizaion noise Phase inerpolaion Inheren fracional divider Inerpolaion jier Pulse generaion Inser pulses Inerpolaion jier PF LPF VCO k mbis ivide by N or N1 Overflow mbi Accumulaor Fig. 12.420

Lecure 170 Frequency Synhesizers I (6/25/03) Page 17019 A 1 GHz FracionalN Frequency Synhesizer Block diagram: PF/CP LPF Mulimodulus Prescaler N2, N1, N, N1, N2, N3 LC VCO Buffer Oupu Conrol nbis N2 N1 N N1 N2 N3 Mode Conrol Logic C 1 C 2 1 C 3 2 ab ab ab Fig. 12.421 Experimenal Resuls: Carrier Phase Noise, Phase Noise, Phase Noise, Phase Noise, Phase Noise, Frequency 10kHz offse 100kHz offse 200kHz offse 600kHz offse 1MHz offse 972 MHz 83.1dBc/Hz 104.1dBc/Hz 110dBc/Hz 188dBc/Hz 122.4dBc/Hz 916MHz 84.6dBc/Hz 104.4dBc/Hz 110.4dBc/Hz 118.2dBc/Hz 122.7dBc/Hz Sideband spurs < 70dBc, power supply range of 2.7 o 4.5V (5.2mA a 3V), uning range 0.881GHz Lecure 170 Frequency Synhesizers I (6/25/03) Page 17020 A LowNoise, 1.6 GHz CMOS Frequency Synhesizer A CMOS PLL used o design he fronend RF funcion of frequency synhesizer. Block iagram: = 61.5MHz PF Charge Pump Loop Filer LC VCO ivide by 1/26 Circui iagram of he LC Oscillaor: C Tune L 1 M1 V Bias M3 M2 I SS V L 2 C var C AC CTune C AC C var R R To Loop Filer Fig. 12.423 Performance: Power supply 2.7V o 5V Power dissipaion a 3V is 90mW Phase noise of 105dBc/Hz a 200kHz offse Tuning range of 1.6GHz±100MHz 1.5mm2 in 0.6µm CMOS echnology Fig. 12.424 J.Parker and.ray, A LowNoise 1.6 GHz CMOS PLL wih OnChip Loop Filer, Proc. of 1997 Conf. on Cusom Inegraed Circuis, May 1997.

Lecure 170 Frequency Synhesizers I (6/25/03) Page 17021 Comparison of Recen CMOS VCO Noise Resuls Auhor Craninckx, Seyar, ISSCC95 Rael, Abidi, ISSCC96 Souyer, ISSCC96 Thamsirianu, CICC94 Weigand, ISCAS94 Parker, Ray, CICC97 Power issipaion P Frequency f 0 Phase Noise o Carrier Raio Offse Freq. (f) Esimaed Open Loop Q 24mW @3V 1.8 GHz 85dBc 10kHz 10 4x1015 43mW@3V 900MHz 100dBc/Hz 100kHz 4 1.7x1015 24mW@3V 4GHz 106dBc/Hz 1MHz 7 1.2x1015 7.5mW@3V 900MHz 93dBc/Hz 100kHz 1 (Class B ring osc.) 0.3x1015 10mW@3V 1GHz 85dBc/Hz 100kHz 1 (Class A ring osc.) 2.5x1015 90mW@3V 1.6GHz 105dBc/Hz 200kHz 7 0.6x1015 Park, CICC98 17mW@3V 980MHz 109dBc/Hz 200kHz 8 0.2x1015 Phase Noise Carrier Ampliude = K f 0 0 f 2 1 PQ K 0 Lecure 170 Frequency Synhesizers I (6/25/03) Page 17022 IVIERS FOR FREQUENCY SYNTHESIZERS Inroducion We have seen ha in he previous maerial ha dividers can be eiher fixed or programmable. In his secion we will focus on circuis and conceps suiable for fixed, ineger and fracionaln dividers. In addiion, we shall consider noiseshaping echniques using delasigma mehods applied o he fracionaln echnique.

Lecure 170 Frequency Synhesizers I (6/25/03) Page 17023 Fixed ividers ToggleFlipflop based divideby2: v osc v osc Q Q v div v div ToggleFlipflop v osc Flipflop Implemenaion: Proper sizing of he ransisors resuls in reasonable powerspeed radeoffs a GHz raes. evice mismaches can resul in phase imbalances as large as 5. If he inpu is no perfecly differenial, addiional phase unbalances can occur. R L M1 Fig. 4.311 V RL M2 M4 M5 Q Q M3 M6 Fig. 4.312 Lecure 170 Frequency Synhesizers I (6/25/03) Page 17024 ual Modulus ividers Evoluion of a divideby2/3 from a divideby3 circui: Q Q 1 1 G Q G 1 FF 1 FF 2 Q 2 Q G Q 2 Fig. 4.313 ivideby2/3 circui (MC=1 2, MC=0 3): N=3 Q FF 1 Q 1 G 1 G FF 2 Q Q 2 Q 1 G MC Fig. 4.314 Q 2 N=2

Lecure 170 Frequency Synhesizers I (6/25/03) Page 17025 ual Modulus ividers Coninued Sae diagram of he divide by 2/3 circui: MC=0 "1" Q 1 Q 2 :00 Q 1 Q 2 :01 2/3 decision poin "X" "1" "0" Q 1 Q 2 :01 "X" Q 1 Q 2 :11 Fig4.3135 Lecure 170 Frequency Synhesizers I (6/25/03) Page 17026 Speed of he ual Modulus ivider The divideby3 circuis are generally much slower han heir dividebywo counerpars. Consider he implemenaion of par of he previous divideby2/3 circui. G 1 V V FF2 R L RL R L RL Q 2 Q2 M1 M2 M1 M2 M4 M5 M3 M3 M6 Fig. 4.315 On he clock edge where Q 2 mus change, sufficien ime mus be allowed for he delay of he AN gae, G 1, and he inpu sage of FF2 before he nex clock ransiion. I is seen ha he delay for 3 circui is nearly wice ha of he 2 circui.

Lecure 170 Frequency Synhesizers I (6/25/03) Page 17027 Programmable ividers A divider can be achieved by using a programmable couner. Preload Inpu (= division raio M) Preload Enable Clock (= ) Programmable Couner, N 2 Maximum coun = N 2 Couner Oupu (= f divide ) For a given speed requiremen, a programmable Fig. 4.316 divider is less power opimized because he criical pah is dependen on he loaded value. A complee divider consising of a fixed divider cascaded wih a programmable divider. fo Fixed Couner N 1 f inermediae Programmable Couner N 2 Max. coun = N 2 (max) f divide Power is high, power can be opimized Power is low, power canno be opimized Fig. 4.317 Resoluion (Complee divider) = Resoluion (programmable divider) x ivision raio (fixed divider) Lecure 170 Frequency Synhesizers I (6/25/03) Page 17028 Waveforms of Various Complee ividers N 1 = 3 and N 2 = 4: f inermediae 3 3 3 3 N 1 = 3 and N 2 = 3: 12 f f divide = /12 divide Fig. 4.318 f inermediae 3 3 3 9 f f divide = /9 divide Fig. 4.319

Lecure 170 Frequency Synhesizers I (6/25/03) Page 17029 Waveforms of Various Complee ividers Coninued N 1 = 3/4 (N 1 = 4 for one N 2 cycle) and N 2 = 3: f inermediae 4 3 3 f divide 10 f divide = /10 Fig. 4.320 N 1 = 3/4 (N 1 = 4 for wo N 2 cycles) and N 2 = 3: f inermediae 4 4 3 11 f f divide = /11 divide Fig. 4.320 Lecure 170 Frequency Synhesizers I (6/25/03) Page 17030 MuliModulus ividers 4/ 5 dual modulus couner example: MC Q1 Q d2 d0 d1 Q f 4, 5 Q Q3 Q2 Sae iagram: Pah B X 0 100 1 4/5 decision poin 000 0 010 110 X Pah A 0 1 Pah B 001 011 X Fig. 4.323 f ps Fig. 4.322 Noe ha here are wo possible sae pahs A and B each consising of wo sequences, a 4 sequence and a 5 sequence. For pah A, he 4 sequence is from 000, 001,011, 010, 000 and he 5 sequence is from 000, 001, 011, 010, 100, 000. For pah B, he 4 sequence is from 000, 001, 011, 110, 000 and he 5 sequence is from 000, 001, 011, 110, 100, 000.

Lecure 170 Frequency Synhesizers I (6/25/03) Page 17031 NOISE SHAPING TECHNIQUES elasigma Shaping Techniques elasigma modulaors can be used along wih mulimodulus dividers o achieve noise shaping of phase noise. The objecive of he delasigma modulaor is o remove he noise due o he flucuaion of he mulimodulus dividers. The following slides review his echnique as applied o frequency synhesizers. Analog implemenaion of a firsorder delasigma modulaor: x() Inegraor 1bi quanizer y(nt) 1bi AC Fig. 4.324 Lecure 170 Frequency Synhesizers I (6/25/03) Page 17032 igial Implemenaion of he elasigma Modulaor Inpu, k mbis Clock 1bi mbis mbis Oupu Residue, R F(z) z1 z1 1bi quanizer A(z) 1 0 2 m Y(z) 2 m 0 Q(z) A(z) Y(z) Fig. 4.325 The discree firsorder delasigma modulaor can be implemened wih an mbi accumulaor. The mbi accumulaor has m inpu bis, a single oupu bi (carrybi or MSB), and mresidue bis. Operaion: On every cycle of he reference clock, he residue oupu R of he accumulaor is assigned he value Rk afer one cycle if an overflow does no occur or he value Rk2 m if he accumulaor produces a carrybi signal. Therefore, he accumulaor overflow is equivalen o he comparaor decision. The daa sored in he accumulaor is essenially he inegral of he error beween he desired frequency daa k and he acual frequency conrol inpu.

Lecure 170 Frequency Synhesizers I (6/25/03) Page 17033 HighOrder elasigma Modulaors zransform of a firsorder delasigma modulaor: Q(z) Inpu F(z) 1 1z1 Y(z) z1 nh order delasigma modulaor: f(n) Fig. 4.326 FirsOrder Sigma ela Modulaor y 1 (n) Q(z) q 1 (n) FirsOrder Sigma ela Modulaor y 2 (n) Bi Manipulaion q 2 (n) FirsOrder Sigma ela Modulaor y 3 (n) Circuiry y(n) Fig. 4.327 q N (n) FirsOrder Sigma y N1 (n) ela Modulaor Lecure 170 Frequency Synhesizers I (6/25/03) Page 17034 Use of a Modulaor for ivider Conrol Consider he secondorder delasigma modulaor implemened wih mbi accumulaors: 1 Adder 1 1 y(n) Bi Manipulaion Circuiry Inpu, k mbis mbis Residue, R mbis mbis Residue, R mbis Fig. 4.328 mbis

Lecure 170 Frequency Synhesizers I (6/25/03) Page 17035 Use of a Modulaor for ivider Conrol Coninued zranform model for he previous secondorder delasigma modulaor: Q 1 (z) Inpu F(z) 1 1z1 Y 1 (z) Y(z) z1 Q 1 (z) Q 2 (z) 1 z1 1z1 Y 2 (z) Fig. 4.329 From he above diagram, we can wrie, Y 1 (z) = F(z) (1z 1 )Q 1 (z) and Y 2 (z) = Q 1 (z)(1z 1 ) Q 2 (z)(1z 1 ) 2 can be combined o give, Y (z) = F(z) Q 2 (z)(1z 1 ) 2 Generalizing o he nh order gives, Y (z) = F(z) Q n (z)(1z 1 ) n z1 Lecure 170 Frequency Synhesizers I (6/25/03) Page 17036 Use of a Modulaor for ivider Conrol Coninued The effecive divide raio of a fracional divider implemened wih an nh order delasigma modulaor can be wrien as, N eff = N(z) Y(z) = N(z) F(z) Q n (z)(1z 1 ) n where N(z) = ineger par of he divide raio F(z) = fracional par of he divide raio Q(z) = quanizaion noise occurring a he nh delasigma modulaor If he PLL is in lock, hen = N eff = [N(z) F(z)] (1z 1 ) n Q n (z) where he firs erm is he desired frequency and he second erm represen he frequency flucuaion resuling from he quanizaion noise in he fracional modulaor.

Lecure 170 Frequency Synhesizers I (6/25/03) Page 17037 Use of a Modulaor for ivider Conrol Coninued Assume ha he quanizaion noise is a random quaniy in he inerval {0.5, 0.5 } wih equal probabiliy. If he quanizer is 1bi, hen which is he quanizaion sep size is 1. The noise power or variance, σ e 2, can be found as 0.5 σ e 2 = E(e) = 1 e 2 de = 2 12 0.5 The specrum of he quanizaion noise is where N(f) is given as, N(f) = 2 12 where is he sampling frequency which is equal o he comparison frequency of he PF. N(f) f Fig. 4.330 Lecure 170 Frequency Synhesizers I (6/25/03) Page 17038 Use of a Modulaor for ivider Conrol Coninued efine f(z) as he frequency noise of flucuaion of he oupu frequency (z). The power specral densiy, S f(z), can be calculaed from he second erm of he previous expression for (z). S f(z) = (1z 1 ) n 2 2 12 = (1z 1 ) n 2 1 12 = (1z 1 ) f 2n ref 12 Because phase is relaed o frequency hrough inegraion, he phase noise, θ n (), is θ n () = 2π f()d Using a simple recangular inegraion in he zdomain yields, 2π f(z) Θ n (z) = (1z 1 ) The power specral densiy of he phase noise, S Θn (z), can be wrien as, S Θn (z) = Θ n (z) 2 (2π) 2 S f(z) = f 2 ref 1z 1 2 S f(z) = (2π)2 1z 1 2(n1) 12 f rads 2 /Hz ref Assuming S Θn (f) is a wosided power specral densiy funcion gives L(f) = S Θn (f) L(f) = (2π)2 12 f πf 2(n1) ref 2sin rads 2 /Hz where z 1 has been replaced wih e j2πf/ and n is he order of he modulaor.

Lecure 170 Frequency Synhesizers I (6/25/03) Page 17039 Use of a Modulaor for ivider Conrol Coninued Prediced phase noise of higherorder modulaors (f sample = 12.8 MHz): Lecure 170 Frequency Synhesizers I (6/25/03) Page 17040 Use of a Modulaor for ivider Conrol Coninued Resuls: If a modulaor has an accumulaor inpu daa k consising of m bis, hen he oscillaor oupu frequency,, can be given as, = N k 2 m The uncerainy of his frequency will be reduced by he use of he sigmadela modulaor. Summary: The delasigma modulaor aenuaes phase noise from he facional conroller o negligible levels close o he cener frequency. Furher from he cener frequency, he phase noise increase rapidly and mus be filered ou prior o uning he inpu of he VCO. The loop filer in he PLL is used o filer he noise away from he cener frequency. When a higherorder, delasigma modulaor is used for a fracionaln conroller, he PLL needs more poles in he loop filer o suppress he quanizaion noise a high frequencies.

Lecure 170 Frequency Synhesizers I (6/25/03) Page 17041 SUMMARY Examine he applicaions of PLLs 1.) emodulaion and modulaion 2.) Signal condiioning 3.) Frequency synhesis 4.) Clock and daa recovery 5.) Frequency ranslaion Inegraed Circui Frequency Synhesizers Archiecures and Techniques Fracional N ividers/prescalers Noise shaping echniques