Introduction to Surface Acoustic Wave (SAW) Devices
|
|
- Edward Briggs
- 5 years ago
- Views:
Transcription
1 April, 8 Introduction to Surface Acoustic Wave (SAW) Devices Part 4: Resonator-Based RF Filters Ken-ya Hashimoto hiba University k.hashimoto@ieee.org
2 ontents Basic Filter Design Ladder Type Filter Design Lattice Filter Design Stacked Resonator Filter Design oupled Resonator Filter Design
3 ontents Basic Filter Design Ladder Type Filter Design Lattice Filter Design Stacked Resonator Filter Design oupled Resonator Filter Design
4 H (db) N-th Order Butterworth Filter Maximally Flat Response: H (n) ()= for n=,,---n H ( ) N ( / ) N=3 N=5-8 N=7 - N= Relative frequency H (db) - N=3 - N=5 N=7-3 N= Relative frequency Gradual Skirt & Group Delay haracteristics
5 S (db) N-th Order hebyshev Filter Equal-Ripple haracteristics (: parameter) H ( ) T N ( / ) cos( N cos hebyshev polynomial T N x) cosh( N cosh -.db -4-6 N=3 N=5-8 N=7 N= Relative frequency S (db) ( - x) x).db N=3 - N=5 N=7 N= Relative frequency Good Skirt but Bad Group Delay haracteristics x x
6 7 Element T-type Butterworth LPF Various values R =5 f =MHz
7 L' ' ' ' L' L' ' L' ' ' L' L' ' L' ' L L LPF to HPF LPF to BPF LPF to BEF / ' / ' L L c c c c ' ', ' ' L L ' ) /( ' ) ( ' ) /( ' ) ( L L L c c c c c c / ' ) /( ' ) ( / ' ) /( ' ) ( L L L c c c c c c ' ', ' ' L L Original LPF (ut-off c )
8 R =5=%, f c =MHz
9 Infinite Q Q= for Parallel-L Q= for Series-L Round Left Shoulder Increased Insertion Loss Round Right Shoulder
10 Influence of Mutual L M L L L -M L -M M V V di L dt di M dt M L di dt di dt ( L ( L di M ) M dt di M ) M dt d dt ( I d ( I dt I I ) )
11 Null Generation! Equivalent to L 4 & L 6 oupling Equivalent to L & L 3 oupling
12 onstant K Filter E S R L L/=R R Uniform Impedance Values V L L L L V I I I L L L I V ascade-onnection with Inversion (Equivalent ircuit for Transmission Line)
13 V L L L L V H = When Equivalent Transmission Line I I Length is n/ H (db) N=3 N=3 N=5 - N=5-8 N=7 N=7 N=9 N= Relative frequency Relative frequency H (db) Similar Response to Butterworth Filter
14 Fabry-Perot Resonator A A T T L Interference Between Two Reflected Waves % Transmit When L=n/
15 Image Parameter Z i, Z o & Z i Z i Z o Z o Z i Z i Z Z o Example Z s ascade onnection with Inversion Z p Z i Z o Z o Z i Z i Z o Z i Z s ( Z s Z p ) F Z i cosh Zi sinh 3 Z o Z i sinh cosh Y o Z o sinh Y Z p s ( Y p / Z Y p s ) where =Z i /Z o
16 Analysis i i i 3 i M+ e e e3 [Fe] e M+ R [Fo] [Fe] [Fo] or [Fo] R e out e in # # #3 #M. ascade onnection with Inversion cosh M Z i sinh M Zi sinh M cosh M F cosh M Zi sinh M Zi sinh M cosh M ( M ( M :odd) :even)
17 i i R e F F e E in R F F S F F R F G F ( )cosh M ( Zi / R cosh M ( Zi / R R R / Zi )sinh / Z )sinh M i M ( M :odd) ( M :even) When jn / M, S =
18 R R L E S L L K j K Z K Z c c c o c i /, / / sin ) / ( / ) / ( When < c Imag., Z i & Z o Real Passband =jn / c =sin(n When > c Real, Z i & Z o Imag. Rejection band Zero Insertion Loss
19 Derived m Filter E S R L R =L/ R onstant K Filter ml (m - -m) m (m - -m)l ml m R =L/ m Null Due to Series Resonance Null Due to Parallel Resonance
20 ml L L ml m (m - -m)l m (m - -m)l ombination of Derived m and onstant K Filters H (db) Relative frequency H (db) Relative frequency Steep Skirt and Good Out-Band Rejection - - m=.6 m=.7 m=.8 m=.9 m=
21 ontents Basic Filter Design Ladder Type Filter Design Lattice Filter Design Stacked Resonator Filter Design oupled Resonator Filter Design
22 Ladder-Type Filter onfiguration (Resonator-Based onstant K Filter) Fabrication of Multiple Resonators on a hip Low Loss High Power Durability Moderate Out-of-Band Rejection
23 Performance of Ladder-Type SAW Filter Scattering Parameter S (db) Tx W-DMA-Rx Rx Frequency (MHz) Fujitsu FAR-F6P-G4-LM Scattering Parameter S (db)
24 - r s - Y s a s Frequency [GHz] Scattering Parameter, S [db]
25 - a p - r p Y p Frequency [GHz] Scattering Parameter, S [db]
26 - Y s Y p Y p r s a p - r p a s Frequency [GHz] Scattering Parameter, S [db]
27 r r r r a a Q j j Q j j j Y ) / / ( ) / ( ) / / ( ) / ( p Resonator Model for Y p & Y s. Q r Identical for Z s Z p. rs = a p Assumption R L Z s Z p s p s p p o o p s s i Y Y Y Y Y Z Y Z Z Z Z / sinh ) ( ) ( Passband When -<Y p /Y s < (Either Y s or Y p Inductive)
28 Relative admittance Y p r p Null Y s a s ap r s Null Passband When -<Y p /Y s < (Either Y s or Y p Inductive) Larger Y s Offers Wide Bandwidth
29 At the Resonance(=) ) ( ) / / ( NrM Z R R Z N S p s s r where s p R Loss Minimum ondition = / Q r M (FOM) s p r / NrM S s r Low Loss When NrM - «:even) ( )sinh / / ( cosh :odd) ( )sinh / / ( )cosh ( M M Z R R Z M M M Z R R Z M S i i i i
30 Bandwidth s r ( )( r ( )( r ) ) r ( )( r where ) p s r / Out-of-Band Rejection When =, S cosh( N) T N r where T N (x)=cosh(ncosh - x): hebyshev Polynomial N Influences IL and OoB Rejection r Influences IL, Bandwidth and OoB Rejection
31 Scattering Parameter, S [db] -5 - N= -5 N= - N=3 N=4-5 r=.4 N= Frequency [GHz]
32 Scattering Parameter, S [db] - - r=.4 N= N= N=3 N=4 N= Frequency [GHz]
33 Scattering Parameter, S [db] -5 - N=5-5 - r=. -5 r=.4-3 r=.6 r=.8-35 r= Frequency [GHz]
34 Scattering Parameter, S [db] - - N=5 r=. r=.4 r=.6 r=.8 r= Frequency [GHz]
35 Scattering Parameter, S [db] N=5 r=.4 =MHz =MHz =4MHz =6MHz =8MHz Frequency [GHz]
36 Scattering Parameter, S [db] N=5 r= d=mhz Q p =, Q s = - Q p =, Q s = Q -.5 p =, Q s = Q p =Q s = Frequency [GHz]
37 Influence of ommon Impedance L i SAW Device hip S S S 3 L o wire SAW chip wire i e P e P e3 P 3 e4 o L e L e L e feedthrough L c Origin of L c Equivalent ircuit
38 Scattering Parameter, S [db] r=.4 =MHz N=5 L c = L c =.nh L c =.nh L c =.3nH Frequency [GHz]
39 Scattering Parameter, S [db] r=.4 =MHz N=5 L c = L c =.nh L c =.nh L c =.3nH Frequency [GHz]
40 Design of Ladder-type Filters Resonator Limits Achievable Band Width For IL Minimization, r p s R S For Wide bandwidth, rs should be a little larger than p a With smaller r= p / s, IL and Band Width Improved but OoB Rejection Deteriorated. With N, OoB Rejection Improved but IL Increases IL is Very Sensitive to Motional Resistance of Y s Very Sensitive to Parasitics Q Influences IL and Shoulder haracteristics
41 ontents Basic Filter Design Ladder Type Filter Design Lattice Filter Design Stacked Resonator Filter Design oupled Resonator Filter Design
42 Lattice Filter Resonator Y o R Y e R e out Balanced I/O e in Y o Y o / Y e / :- Equivalent ircuit Unbalanced I/O
43 Y o -Y e Y o -Y e Y e -Y o Y e -Y o :- Y e Y e Y o Y o Modified Equivalent ircuit Equivalent to -Stage ascaded L-type (or -type) Filter Res. Freq. for Series Arm Anti-Res. Freq. for Parallel Arm Y e =, Y o = or Y o =, Y e =
44 Resonance ondition Res. Freq. for Y o Anti-Res. Freq. for Y e Or Res. Freq. for Y e Anti-Res. Freq. for Y o S R ( Yo Ye ) ( Y R )( Y e o R ) At Resonance ( M S o r ( M M ) M ) IL Min. ondition Where M=Q r / R S o r M M
45 Frequency Response S (db) Y o 5 - Y e S Relative frequency Good OoB Rejection Relative admittance (db)
46 Wideband When ro > a e -5 - S (db) S (db) Relative frequency -3-4 = =.% =.4% =.6%
47 Better OoB Rejection When o > e - S (db) Relative frequency r= r=.95 r=.9 r=.85 r=.8 Null Generation Near Passband
48 Relative admittance Y e r o Y o a e ao r e S R ( Yo Ye ) ( Y R )( Y e o R ) Null Generation When Y e =Y o
49 Influence of Mutual oupling L I SAW Device L L I c V L 4 L 3 L 3 L L 4 33 L 44 I 3 I 4 L 34 V Very Small Values but May Not Negligible
50 Influence of Inductive oupling EM Feedthrough (db) = =3.5pF (b) c =.5fF, L 34 =.5pH (a) c =.5fF Frequency (GHz) Tiny oupling Gives Significant Influence
51 ontents Basic Filter Design Ladder Type Filter Design Lattice Filter Design Stacked Resonator Filter Design oupled Resonator Filter Design
52 Stacked FBAR Filter Electrodes Si Good OoB Rejection Moderate IL L m m R m R Z R Equivalent ircuit for Fundamental Resonance E Static apacitance When Parallel-onnected -Port Resonator When Parallel-onnected with Inversion
53 Frequency Response of Stacked Resonator Filter From TFR Technologies 53
54 i L m m R m e e Transfer Function S ( j R Z i ){ ZR ( i i Where j R Y Y Y Y Z ) } Y Y j Z jl e e m Z R m / j m Ideal ase (R m =), ZR ( j R ) /( j R ) At Satisfying S j R j R Z ( R S jr ) (Loss Less)
55 }] ) ( /{ / ) ( [ ) ( G G R L j j G G S m ) ( ) ( R R j R L j Z m Gives }/ ) ( { R R R S m M R S m R IL Min. ondition / / Q M R L R Q m m m m m Determined by M
56 ] ) / ( [ M j j S G When ] [ M S ] ) / ( [ M -3dB Bandwidth ) ( M S / / Q M R L R Q m m m m m When Determined by M and
57 Response of Stacked Resonator Filter S [db] R = R = Frequency [GHz] ZnO (L=.6 m, S=66 m ) S is Set to Z-Match at GHz
58 ascaded Stacked Resonator Filters L m m R m L m m R m L m m R m R R E in R R E in F N jr jr cos e cos N e sin sin N jre sin cos N jre sin N cos N where cos jr jr e e Z sin Z sin jl m j j R m Z / ( j j m Z)
59 S [db] N= N= N=3 N= Frequency [GHz] ZnO (L=.6 m, S=66 m ) Widened Passband Steeper Skirt haracteristics
60 ontents Basic Filter Design Ladder Type Filter Design Lattice Filter Design Stacked Resonator Filter Design oupled Resonator Filter Design
61 Uncoupled State k M M k Resonance Frequency: r =(k/m).5 oupled State k M k c M k Resonance Frequency Symmetric Resonance: rs ={(k+k c )/M}.5 Antisymmetric Resonance: ra =(k/m).5
62 oupled Resonator + + M M V - dv dt dv dt v i v v k k v v M k - dt dt k - k c k c M ( v ( v V - v v ) dt ) dt v i V V V F k c - F V (a) Electric + Mechanical ircuit
63 i v M k - k - M v i V F k c - F V (a) Electric + Mechanical ircuit M k - k - M k c - (b) Mechanical ircuit
64 M k - k - M k c - M k - k - M (k c ) - (k c ) - (a) Symmetric Resonance M k - k - M (b) Antisymmetric Resonance
65 Transversally oupled Double-Mode Filter Electrodes Si Symmetrical & Antisymmetrical Resonances R in E in L m L m a m a s m s a R m s R m :- Equivalent ircuit R out -Port Resonator When Parallel- onnected Another -Port Resonator When Parallel-onnected with Inversion
66 Equivalent ircuit of Double-Mode Filter Y e =(Y me +j ) Y o =(Y mo +j ) Y me, Y mo :Motional Y, j :Static apacitances Equivalent to Lattice Filter Y mo / Y me / :- Y o / Y e / :-
67 Design Principle of Wideband DMS Filters oincidence of Multiple Resonance for Y e (or Y o ) with Antiresonance for Y o (or Y e ) r o a o r e e a r o a o Employing More Resonances Results in More Bandwidths
68 Double Mode SAW (DMS) Filter Scattering parameter. S [db] Frequency [MHz] Symmetrical & Anti-symmetrical Resonances Scattering parameter. S [db] Fujitsu FAR-F5EB-94M5-B8E
69 oupled Resonator Filter (RF) Input Output Si S [db] Overcoupling -5 - riticalcoupling -5 - Undercoupling Frequency [GHz] ZnO (L=.6 m, S= m ) oupler R=GRayls (Very hard),.8 How to Realize?
70 S [db] S [db] N= -8 N= N= Frequency [GHz] N= - N= N= Frequency [GHz] ascaded RF ZnO (L=.6 m, S= m ) oupler GRayls,.8 Extremely hard ZnO (L=.6 m, S=66 m ) oupler MRayls,. Extremely soft
71 Design of oupled Resonator Filters Band Width Governed by For Loss Minimization, r R S oupling Layer Should be Designed to Adjust Multiple Poles to oincide with Nulls (But Very ritical!) Slight Difference Between Poles & Nulls Effective ascade-onnection is Effective IL is Sensitive to Motional Resistances & Parasitics
Introduction to Surface Acoustic Wave (SAW) Devices
Introduction to Surface Acoustic Wave (SAW) Devices Part 4: Resonator-Based Filters Ken-ya Hashimoto Chiba University k.hashimoto@ieee.org http://www.em.eng.chiba-u.jp/~ken Contents Basic Resonator Theory
More informationInternational Distinguished Lecturer Program
U 005-006 International Distinguished Lecturer Program Ken-ya Hashimoto Chiba University Sponsored by The Institute of Electrical and Electronics Engineers (IEEE) Ultrasonics, Ferroelectrics and Frequency
More informationCase Study: Parallel Coupled- Line Combline Filter
MICROWAVE AND RF DESIGN MICROWAVE AND RF DESIGN Case Study: Parallel Coupled- Line Combline Filter Presented by Michael Steer Reading: 6. 6.4 Index: CS_PCL_Filter Based on material in Microwave and RF
More informationSpeaker: Arthur Williams Chief Scientist Telebyte Inc. Thursday November 20 th 2008 INTRODUCTION TO ACTIVE AND PASSIVE ANALOG
INTRODUCTION TO ACTIVE AND PASSIVE ANALOG FILTER DESIGN INCLUDING SOME INTERESTING AND UNIQUE CONFIGURATIONS Speaker: Arthur Williams Chief Scientist Telebyte Inc. Thursday November 20 th 2008 TOPICS Introduction
More information192 Chapter 4: Microwave Network Analysis
92 hapter 4: Microwave Network nalysis TLE 4.2 onversions etween Two-Port Network Parameters S Z Y S S (Z Z 0 )(2 + Z 0 ) (Y 0 Y )(Y 0 + Y 22 ) + Y 2 Y 2 + /Z 0 Z 0 + /Z 0 + Z 0 + S S 2Z 2 Z 0 2 2 2Y 2
More informationFilters and Tuned Amplifiers
Filters and Tuned Amplifiers Essential building block in many systems, particularly in communication and instrumentation systems Typically implemented in one of three technologies: passive LC filters,
More informationInternational Distinguished Lecturer Program
U 005-006 International Distinguished Lecturer Program Ken-ya Hashimoto Chiba University Sponsored by The Institute of Electrical and Electronics Engineers (IEEE) Ultrasonics, Ferroelectrics and Frequency
More informationLectures: Lumped element filters (also applies to low frequency filters) Stub Filters Stepped Impedance Filters Coupled Line Filters
ECE 580/680 Microwave Filter Design Lectures: Lumped element filters (also applies to low frequency filters) Stub Filters Stepped Impedance Filters Coupled Line Filters Lumped Element Filters Text Section
More informationElectronic Circuits EE359A
Electronic Circuits EE359A Bruce McNair B26 bmcnair@stevens.edu 21-216-5549 Lecture 22 569 Second order section Ts () = s as + as+ a 2 2 1 ω + s+ ω Q 2 2 ω 1 p, p = ± 1 Q 4 Q 1 2 2 57 Second order section
More informationSolutions to Problems in Chapter 6
Appendix F Solutions to Problems in Chapter 6 F.1 Problem 6.1 Short-circuited transmission lines Section 6.2.1 (book page 193) describes the method to determine the overall length of the transmission line
More informationCharacteristic of Capacitors
3.5. The Effect of Non ideal Capacitors Characteristic of Capacitors 12 0 (db) 10 20 30 capacitor 0.001µF (1000pF) Chip monolithic 40 two-terminal ceramic capacitor 0.001µF (1000pF) 2.0 x 1.25 x 0.6 mm
More informationDesign Considerations on Wideband Longitudinally-Coupled Double-Mode SAW Filters
Design Considerations on Wideb Longitudinally-Coupled Double-Mode SAW Filters Ken-ya Hashimoto, Tatsuya Omori Masatsune Yamaguchi Dept. of Electronic Mechanical Eng., Chiba University Abstract This paper
More informationElectronic Circuits EE359A
Electronic Circuits EE359A Bruce McNair B26 bmcnair@stevens.edu 21-216-5549 Lecture 22 578 Second order LCR resonator-poles V o I 1 1 = = Y 1 1 + sc + sl R s = C 2 s 1 s + + CR LC s = C 2 sω 2 s + + ω
More informationPaper V. Acoustic Radiation Losses in Busbars. J. Meltaus, S. S. Hong, and V. P. Plessky J. Meltaus, S. S. Hong, V. P. Plessky.
Paper V Acoustic Radiation Losses in Busbars J. Meltaus, S. S. Hong, and V. P. Plessky 2006 J. Meltaus, S. S. Hong, V. P. Plessky. V Report TKK-F-A848 Submitted to IEEE Transactions on Ultrasonics, Ferroelectrics,
More informationSYNTHESIS OF MICROWAVE RESONATOR DIPLEX- ERS USING LINEAR FREQUENCY TRANSFORMATION AND OPTIMIZATION
Progress In Electromagnetics Research, Vol. 24, 44 4, 22 SYNTHESIS OF MICROWAVE RESONATOR DIPLEX- ERS USING LINEAR FREQUENCY TRANSFORMATION AND OPTIMIZATION R. Wang *, J. Xu, M.-Y. Wang, and Y.-L. Dong
More informationA Novel Tunable Dual-Band Bandstop Filter (DBBSF) Using BST Capacitors and Tuning Diode
Progress In Electromagnetics Research C, Vol. 67, 59 69, 2016 A Novel Tunable Dual-Band Bandstop Filter (DBBSF) Using BST Capacitors and Tuning Diode Hassan Aldeeb and Thottam S. Kalkur * Abstract A novel
More informationHigh Speed Communication Circuits and Systems Lecture 4 Generalized Reflection Coefficient, Smith Chart, Integrated Passive Components
High Speed Communication Circuits and Systems Lecture 4 Generalized Reflection Coefficient, Smith Chart, Integrated Passive Components Michael H. Perrott February 11, 2004 Copyright 2004 by Michael H.
More informationApplications of Ferroelectrics for Communication Antennas
Applications of Ferroelectrics for Communication Antennas HRL Research Laboratories Microelectronics Laboratory Jonathan Lynch, jjlynch@hrl.com Joe Colburn, colburn@hrl.com Dave Laney, dclaney@hrl.com
More informationDigital Integrated Circuits A Design Perspective
Designing ombinational Logic ircuits dapted from hapter 6 of Digital Integrated ircuits Design Perspective Jan M. Rabaey et al. opyright 2003 Prentice Hall/Pearson 1 ombinational vs. Sequential Logic In
More informationPART TOP VIEW. Maxim Integrated Products 1
9-96; Rev ; 2/ 45, SPDT Analog Switch in SOT23-8 General Description The is a dual-supply, single-pole/doublethrow (SPDT) analog switch. On-resistance is 45 max and flat (7 max) over the specified signal
More informationDesign of all-pole microwave filters. Giuseppe Macchiarella Polytechnic of Milan, Italy Electronic and Information Department
Design of all-pole microwave filters Giuseppe Macchiarella Polytechnic of Milan, Italy Electronic and Information Department In-line filters with all-equal resonators R L eq, f L eq, f L eq, f L eq, f
More informationDiscrete-Time Filter (Switched-Capacitor Filter) IC Lab
Discreteime Filter (Switchedapacitor Filter) I Lab Discreteime Filters AntiAliasing Filter & Smoothing Filter f pass f stop A attenuation FIR Filters f max Windowing (Kaiser), Optimization 0 f s f max
More informationChapter 7: Filter Design 7.1 Practical Filter Terminology
hapter 7: Filter Design 7. Practical Filter Terminology Analog and digital filters and their designs constitute one of the major emphasis areas in signal processing and communication systems. This is due
More informationBME/ISE 3511 Bioelectronics - Test Six Course Notes Fall 2016
BME/ISE 35 Bioelectronics - Test Six ourse Notes Fall 06 Alternating urrent apacitive & Inductive Reactance and omplex Impedance R & R ircuit Analyses (D Transients, Time onstants, Steady State) Electrical
More informationIRGPC40UD2 UltraFast CoPack IGBT
INSULATED GATE BIPOLAR TRANSISTOR WITH ULTRAFAST SOFT REOVERY DIODE PD - 9.88A UltraFast opack IGBT Features Switching-loss rating includes all "tail" losses HEXFRED TM soft ultrafast diodes Optimized
More informationDigital Microelectronic Circuits ( )
Digital Microelectronic ircuits (361-1-3021 ) Presented by: Dr. Alex Fish Lecture 5: Parasitic apacitance and Driving a Load 1 Motivation Thus far, we have learned how to model our essential building block,
More informationPrecision, Quad, SPDT, CMOS Analog Switch
19-0189; Rev 1; 6/99 Precision, Quad, SPDT, MOS Analog Switch General Description The is a precision, quad, single-pole doublethrow (SPDT) analog switch. The four independent switches operate with bipolar
More informationON THE USE OF GEGENBAUER PROTOTYPES IN THE SYNTHESIS OF WAVEGUIDE FILTERS
Progress In Electromagnetics Research C, Vol. 18, 185 195, 2011 ON THE USE OF GEGENBAUER PROTOTYPES IN THE SYNTHESIS OF WAVEGUIDE FILTERS L. Cifola, A. Morini, and G. Venanzoni Dipartimento di Ingegneria
More informationEECS240 Spring Today s Lecture. Lecture 2: CMOS Technology and Passive Devices. Lingkai Kong EECS. EE240 CMOS Technology
EECS240 Spring 2013 Lecture 2: CMOS Technology and Passive Devices Lingkai Kong EECS Today s Lecture EE240 CMOS Technology Passive devices Motivation Resistors Capacitors (Inductors) Next time: MOS transistor
More informationOPERATIONAL AMPLIFIER APPLICATIONS
OPERATIONAL AMPLIFIER APPLICATIONS 2.1 The Ideal Op Amp (Chapter 2.1) Amplifier Applications 2.2 The Inverting Configuration (Chapter 2.2) 2.3 The Non-inverting Configuration (Chapter 2.3) 2.4 Difference
More informationRapid SAW Sensor Development Tools
Rapid SAW Sensor Development Tools W. (Cy) Wilson NASA Langley Research Center G. M. Atkinson Virginia Commonwealth University Outline Motivation Introduction to Surface Acoustic Wave Devices Approach
More informationNetwork Parameters of a Two-Port Filter
Contents Network Parameters of a Two-Port Filter S Parameters in the s-domain Relation between ε and ε R 2 2 Derivation of S 22 3 2 Network Parameters in the jω-domain 3 2 S Parameters in the jω-domain
More informationDesign of SPUDT and RSPUDT SAW Filters
Dr. A.S.Rukhlenko Design of SPUDT and RSPUDT SAW Filters Rukhlenko@bluewin.ch www.intrasaw.com Neuchâtel, 2005 1 Outline Introduction 1. Single Phase Unidirectional SAW Transducer (SPUDT) 2. SPUDT Design
More informationDesign of Narrow Band Filters Part 2
E.U.I.T. Telecomunicación 200, Madrid, Spain, 27.09 30.09.200 Design of Narrow Band Filters Part 2 Thomas Buch Institute of Communications Engineering University of Rostock Th. Buch, Institute of Communications
More informationCharacteristics of Passive IC Devices
008/Oct 8 esistors Characteristics of Passive IC Devices Poly esistance Diffusion esistance Well esistance Parasitic esistance Capacitors Poly Capacitors MOS Capacitors MIM Capacitors Parasitic Capacitors
More informationElectronic Circuits Summary
Electronic Circuits Summary Andreas Biri, D-ITET 6.06.4 Constants (@300K) ε 0 = 8.854 0 F m m 0 = 9. 0 3 kg k =.38 0 3 J K = 8.67 0 5 ev/k kt q = 0.059 V, q kt = 38.6, kt = 5.9 mev V Small Signal Equivalent
More informationCMOS Cross Section. EECS240 Spring Dimensions. Today s Lecture. Why Talk About Passives? EE240 Process
EECS240 Spring 202 CMOS Cross Section Metal p - substrate p + diffusion Lecture 2: CMOS Technology and Passive Devices Poly n - well n + diffusion Elad Alon Dept. of EECS EECS240 Lecture 2 4 Today s Lecture
More informationINTC 1307 Instrumentation Test Equipment Teaching Unit 6 AC Bridges
IHLAN OLLEGE chool of Engineering & Technology ev. 0 W. lonecker ev. (8/6/0) J. Bradbury INT 307 Instrumentation Test Equipment Teaching Unit 6 A Bridges Unit 6: A Bridges OBJETIVE:. To explain the operation
More informationCharacteristic Symbol Value Unit Output Current I out 150 ma
LBNB ma LOAD SWITH FEATURING OMPLEMENTARY BIPOLAR TRANSISTORS NEW PRODUT General Description LMNB is best suited for applications where the load needs to be turned on and off using control circuits like
More informationPoles and Zeros in z-plane
M58 Mixed Signal Processors page of 6 Poles and Zeros in z-plane z-plane Response of discrete-time system (i.e. digital filter at a particular frequency ω is determined by the distance between its poles
More informationAC Circuits. The Capacitor
The Capacitor Two conductors in close proximity (and electrically isolated from one another) form a capacitor. An electric field is produced by charge differences between the conductors. The capacitance
More informationIGBT Designer s Manual
IGBT Designer s Manual Data Sheets The IGBT devices listed in this Designer s Manual represent International Rectifier s IGBT line as of August, 994. The data presented in this manual supersedes all previous
More informationEE105 - Fall 2005 Microelectronic Devices and Circuits
EE5 - Fall 5 Microelectronic Device and ircuit Lecture 9 Second-Order ircuit Amplifier Frequency Repone Announcement Homework 8 due tomorrow noon Lab 7 next week Reading: hapter.,.3. Lecture Material Lat
More informationDigital Control & Digital Filters. Lectures 21 & 22
Digital Controls & Digital Filters Lectures 2 & 22, Professor Department of Electrical and Computer Engineering Colorado State University Spring 205 Review of Analog Filters-Cont. Types of Analog Filters:
More informationECE 410 DIGITAL SIGNAL PROCESSING D. Munson University of Illinois Chapter 12
. ECE 40 DIGITAL SIGNAL PROCESSING D. Munson University of Illinois Chapter IIR Filter Design ) Based on Analog Prototype a) Impulse invariant design b) Bilinear transformation ( ) ~ widely used ) Computer-Aided
More informationCMOS Comparators. Kyungpook National University. Integrated Systems Lab, Kyungpook National University. Comparators
IsLab Analog Integrated ircuit Design OMP-21 MOS omparators כ Kyungpook National University IsLab Analog Integrated ircuit Design OMP-1 omparators A comparator is used to detect whether a signal is greater
More information2 Signal Frequency and Impedances First Order Filter Circuits Resonant and Second Order Filter Circuits... 13
Lecture Notes: 3454 Physics and Electronics Lecture ( nd Half), Year: 7 Physics Department, Faculty of Science, Chulalongkorn University //7 Contents Power in Ac Circuits Signal Frequency and Impedances
More information04 Matching Networks. Dipl.-Ing. Dr. Michael Gebhart, MSc
04 Matching Networks 4th unit in course 3, F Basics and omponents ipl.-ing. r. Michael Gebhart, Mc FI Qualification Network, University of pplied ciences, ampus W 013/14, eptember 30 th ontent Introduction:
More informationExercise s = 1. cos 60 ± j sin 60 = 0.5 ± j 3/2. = s 2 + s + 1. (s + 1)(s 2 + s + 1) T(jω) = (1 + ω2 )(1 ω 2 ) 2 + ω 2 (1 + ω 2 )
Exercise 7 Ex: 7. A 0 log T [db] T 0.99 0.9 0.8 0.7 0.5 0. 0 A 0 0. 3 6 0 Ex: 7. A max 0 log.05 0 log 0.95 0.9 db [ ] A min 0 log 40 db 0.0 Ex: 7.3 s + js j Ts k s + 3 + j s + 3 j s + 4 k s + s + 4 + 3
More informationFull Adder Ripple Carry Adder Carry-Look-Ahead Adder Manchester Adders Carry Select Adder
Outline E 66 U Resources: dders & Multipliers Full dder Ripple arry dder arry-look-head dder Manchester dders arry Select dder arry Skip dder onditional Sum dder Hybrid Designs leksandar Milenkovic E-mail:
More informationImpedance Matching and Tuning
C h a p t e r F i v e Impedance Matching and Tuning This chapter marks a turning point, in that we now begin to apply the theory and techniques of previous chapters to practical problems in microwave engineering.
More informationOp-Amp Circuits: Part 3
Op-Amp Circuits: Part 3 M. B. Patil mbpatil@ee.iitb.ac.in www.ee.iitb.ac.in/~sequel Department of Electrical Engineering Indian Institute of Technology Bombay Introduction to filters Consider v(t) = v
More informationFerroelectrics. Spartak Gevorgian. Department of Microtechnology and Nanoscience Chalmers University of Technology Gothenburg, Sweden
Ferroelectrics Material Properties, Processing, and Microwave Applications Spartak Gevorgian Department of Microtechnology and Nanoscience Chalmers University of Technology Gothenburg, Sweden Norwegian
More informationPreamplifier in 0.5µm CMOS
A 2.125 Gbaud 1.6kΩ Transimpedance Preamplifier in 0.5µm CMOS Sunderarajan S. Mohan Thomas H. Lee Center for Integrated Systems Stanford University OUTLINE Motivation Shunt-peaked Amplifier Inductor Modeling
More informationDesign of IIR filters
Design of IIR filters Standard methods of design of digital infinite impulse response (IIR) filters usually consist of three steps, namely: 1 design of a continuous-time (CT) prototype low-pass filter;
More informationPower Distribution Network Design for High-Speed Printed Circuit Boards
Power Distribution Network Design for High-Speed Printed Circuit Boards Jun Fan NCR Corporation 1 Outline Overview of PDN design in multi-layer PCBs Interconnect Inductance Individual Capacitor Values
More informationCMOS Cross Section. EECS240 Spring Today s Lecture. Dimensions. CMOS Process. Devices. Lecture 2: CMOS Technology and Passive Devices
EECS240 Spring 2008 CMOS Cross Section Metal p - substrate p + diffusion Lecture 2: CMOS echnology and Passive Devices Poly n - well n + diffusion Elad Alon Dept. of EECS EECS240 Lecture 2 4 oday s Lecture
More informationRefinements to Incremental Transistor Model
Refinements to Incremental Transistor Model This section presents modifications to the incremental models that account for non-ideal transistor behavior Incremental output port resistance Incremental changes
More informationDual 4-Input AND Gate
TENIAL DATA Dual 4-Input AND ate The is high-speed Si-gate MOS device and is pin compatible with low power Schottky TTL (LSTTL). The device provide the Dual 4-input AND function. Outputs Directly Interface
More informationUnderstanding EMC Basics
1of 7 series Webinar #1 of 3, February 27, 2013 EM field theory, and 3 types of EM analysis Webinar Sponsored by: EurIng CEng, FIET, Senior MIEEE, ACGI AR provides EMC solutions with our high power RF/Microwave
More informationDesign of Narrow Band Filters Part 1
E.U.I.T. Telecomunicación 2010, Madrid, Spain, 27.09 30.09.2010 Design of Narrow Band Filters Part 1 Thomas Buch Institute of Communications Engineering University of Rostock Th. Buch, Institute of Communications
More informationSynthesis of passband filters with asymmetric transmission zeros
Synthesis of passband filters with asymmetric transmission zeros Giuseppe Macchiarella Polytechnic of Milan, Italy Electronic and Information Department Passband filters with asymmetric zeros Placing asymmetric
More informationand Ee = E ; 0 they are separated by a dielectric material having u = io-s S/m, µ, = µ, 0
602 CHAPTER 11 TRANSMISSION LINES 11.10 Two identical pulses each of magnitude 12 V and width 2 µs are incident at t = 0 on a lossless transmission line of length 400 m terminated with a load. If the two
More informationChapter 6 Objectives
hapter 6 Engr8 ircuit Analysis Dr urtis Nelson hapter 6 Objectives Understand relationships between voltage, current, power, and energy in inductors and capacitors; Know that current must be continuous
More informationSwitched Capacitor Filters (SCF)
Switched apacitor Filters SF) Passive Filters omponents are R, L, Big, Heavy, discrete Inductors are limited in quality Designed in sdomain Active R filters omponents are Opamps, OTAs, R s and s an be
More informationThe Approximation Problem
EE 508 Lecture The Approximation Problem Classical Approximating Functions - Elliptic Approximations - Thompson and Bessel Approximations Review from Last Time Chebyshev Approximations T Type II Chebyshev
More informationStatic CMOS Circuits
Static MOS ircuits l onventional (ratio-less) static MOS» overed so far l Ratio-ed logic (depletion load, pseudo nmos) l ass transistor logic ombinational vs. Sequential Logic In Logic ircuit In Logic
More informationCHAPTER.6 :TRANSISTOR FREQUENCY RESPONSE
CHAPTER.6 :TRANSISTOR FREQUENCY RESPONSE To understand Decibels, log scale, general frequency considerations of an amplifier. low frequency analysis - Bode plot low frequency response BJT amplifier Miller
More informationUNIT - III PART A. 2. Mention any two techniques for digitizing the transfer function of an analog filter?
UNIT - III PART A. Mention the important features of the IIR filters? i) The physically realizable IIR filters does not have linear phase. ii) The IIR filter specification includes the desired characteristics
More informationTHEORY AND REALIZATION OF SIMPLE BANDPASS FILTERS WITH ANTIPARALLEL CONFIGURATION
Progress In Electromagnetics Research, Vol. 136, 101 122, 2013 THEORY AND REALIZATION OF SIMPLE BANDPASS FILTERS WITH ANTIPARALLEL CONFIGURATION Sinisa Jovanovic 1, *, Bratislav Milovanovic 2, and Miodrag
More informationPOWER SUPPLY INDUCED JITTER MODELING OF AN ON- CHIP LC OSCILLATOR. Shahriar Rokhsaz, Jinghui Lu, Brian Brunn
POWER SUPPY INDUED JITTER MODEING OF AN ON- HIP OSIATOR Shahriar Rokhsaz, Jinghui u, Brian Brunn Rockethips Inc. (A Xilinx, Inc. Division) ABSTRAT This paper concentrates on developing a closed-form small
More informationTC 412 Microwave Communications. Lecture 6 Transmission lines problems and microstrip lines
TC 412 Microwave Communications Lecture 6 Transmission lines problems and microstrip lines RS 1 Review Input impedance for finite length line Quarter wavelength line Half wavelength line Smith chart A
More informationIMPEDANCE and NETWORKS. Transformers. Networks. A method of analysing complex networks. Y-parameters and S-parameters
IMPEDANCE and NETWORKS Transformers Networks A method of analysing complex networks Y-parameters and S-parameters 1 ENGN4545/ENGN6545: Radiofrequency Engineering L#7 Transformers Combining the effects
More informationECE 202 Fall 2013 Final Exam
ECE 202 Fall 2013 Final Exam December 12, 2013 Circle your division: Division 0101: Furgason (8:30 am) Division 0201: Bermel (9:30 am) Name (Last, First) Purdue ID # There are 18 multiple choice problems
More informationPrecision, Quad, SPST Analog Switches
9-8; Rev ; 9/ Precision, Quad, SPST Analog Switches General Description The are precision, quad, single-pole single-throw (SPST) analog switches. The MAX364 has four normally closed (N), and the MAX365
More informationAnalysis and Design of Differential LNAs with On-Chip Transformers in 65-nm CMOS Technology
Analysis and Design of Differential LNAs with On-Chip Transformers in 65-nm CMOS Technology Takao Kihara, Shigesato Matsuda, Tsutomu Yoshimura Osaka Institute of Technology, Japan June 27, 2016 2 / 16
More informationTriple 3-Input NOR Gate
TENIAL DATA IN4T2A Triple 3-Input NOR ate The IN4T2A is high-speed Si-gate MOS device and is pin compatible with low power Schottky TTL (LSTTL). The device provide the Triple 3-input NOR function. Outputs
More informationEE221 Circuits II. Chapter 14 Frequency Response
EE22 Circuits II Chapter 4 Frequency Response Frequency Response Chapter 4 4. Introduction 4.2 Transfer Function 4.3 Bode Plots 4.4 Series Resonance 4.5 Parallel Resonance 4.6 Passive Filters 4.7 Active
More informationAn example of answers for the final report of Electronics"
An example of answers for the final report of Electronics" Shingo Katsumoto February 7, 07 Here is an example of answers. There are many other possibilities. DA conversion circuits. Resistance-ladder type
More informationQuartz Crystal Resonator Parameter Calculation Based on Impedance Analyser Measurement Using GRG Nonlinear Solver
16 Quartz Crystal Resonator Parameter Calculation Based on Impedance Analyser Measurement Quartz Crystal Resonator Parameter Calculation Based on Impedance Analyser Measurement Using GRG Nonlinear Solver
More informationELG4125: Power Transmission Lines Steady State Operation
ELG4125: Power Transmission Lines Steady State Operation Two-Port Networks and ABCD Models A transmission line can be represented by a two-port network, that is a network that can be isolated from the
More informationEE221 Circuits II. Chapter 14 Frequency Response
EE22 Circuits II Chapter 4 Frequency Response Frequency Response Chapter 4 4. Introduction 4.2 Transfer Function 4.3 Bode Plots 4.4 Series Resonance 4.5 Parallel Resonance 4.6 Passive Filters 4.7 Active
More informationEquivalent Circuit Model Extraction for Interconnects in 3D ICs
Equivalent Circuit Model Extraction for Interconnects in 3D ICs A. Ege Engin Assistant Professor, Department of ECE, San Diego State University Email: aengin@mail.sdsu.edu ASP-DAC, Jan. 23, 213 Outline
More informationLow-Sensitivity, Highpass Filter Design with Parasitic Compensation
Low-Sensitivity, Highpass Filter Design with Parasitic Compensation Introduction This Application Note covers the design of a Sallen-Key highpass biquad. This design gives low component and op amp sensitivities.
More informationPS391/PS392/PS393. Precision, Quad, SPST, Analog Switches. Description
PS39/PS39/PS393 379379379379379379379379379379379379379 Precision, Quad, SPST, Analog Switches Features Low On-Resistance, ohms typ) Minimizes Disttion and Err oltages On-Resistance Match Between hannels,
More informationLecture 13 Date:
ecture 13 Date: 29.02.2016 Quarter-wave Impedance Transformer The Theory of Small Reflections The Quarter Wave Transformer (contd.) The quarter-wave transformer is simply a transmission line with characteristic
More informationIRGPC50F Fast Speed IGBT
INSULATED GATE BIPOLAR TRANSISTOR PD - 9.695A Fast Speed IGBT Features Switching-loss rating includes all "tail" losses Optimized for medium operating frequency ( to khz) See Fig. for urrent vs. Frequency
More information(1) The open and short circuit required for the Z and Y parameters cannot usually be
ECE 580 Network Theory Scattering Matrix 76 The Scattering Matrix Motivation for introducing the SM: () The open and short circuit required for the Z and Y parameters cannot usually be implemented in actual
More informationPOWER DISTRIBUTION SYSTEM Calculating PDS Impedance Douglas Brooks Ultracad Design, Inc
POWER DISTRIBUTION SYSTEM Calculating PDS Impedance Douglas Brooks Ultracad Design, Inc On a PCB (Printed Circuit Board) the Power Distribution System (PDS) is the system that distributes power from the
More informationSophomore Physics Laboratory (PH005/105)
CALIFORNIA INSTITUTE OF TECHNOLOGY PHYSICS MATHEMATICS AND ASTRONOMY DIVISION Sophomore Physics Laboratory (PH5/15) Analog Electronics Active Filters Copyright c Virgínio de Oliveira Sannibale, 23 (Revision
More informationNumerical and Experimental Analysis of the Parameters of an Electroacoustic Thin-Film Microwave Resonator
ISSN 163-771, Acoustical Physics, 13, Vol. 59, No. 5, pp. 513 5. Pleiades Publishing, Ltd., 13. Original Russian Text M.Yu. Dvoesherstov, V.I. Cherednik, S.I. Bosov, I.Ya. Orlov, O.V. Rudenko, 13, published
More information2GHz Microstrip Low Pass Filter Design with Open-Circuited Stub
IOSR Journal of Electronics and Communication Engineering (IOSR-JECE) e-issn: 2278-2834,p- ISSN: 2278-8735.Volume 13, Issue 2, Ver. II (Mar. - Apr. 2018), PP 01-09 www.iosrjournals.org 2GHz Microstrip
More informationCore Technology Group Application Note 3 AN-3
Measuring Capacitor Impedance and ESR. John F. Iannuzzi Introduction In power system design, capacitors are used extensively for improving noise rejection, lowering power system impedance and power supply
More informationEE482: Digital Signal Processing Applications
Professor Brendan Morris, SEB 3216, brendan.morris@unlv.edu EE482: Digital Signal Processing Applications Spring 2014 TTh 14:30-15:45 CBC C222 Lecture 05 IIR Design 14/03/04 http://www.ee.unlv.edu/~b1morris/ee482/
More informationKeysight Technologies Heidi Barnes
Keysight Technologies 2018.03.29 Heidi Barnes 1 S I G N A L I N T E G R I T Y A N D P O W E R I N T E G R I T Y Hewlett-Packard Agilent Technologies Keysight Technologies Bill and Dave s Company and the
More informationTHEORETICAL EXAMINATION OF ELECTROMAG- NETIC WAVE TUNNELING THROUGH CASCADED ɛ-
Progress In Electromagnetics Research B, Vol. 4, 1, 01 THEORETICAL EXAMINATION OF ELECTROMAG- NETIC WAVE TUNNELING THROUGH CASCADED ɛ- AND µ-negative METAMATERIAL SLABS C. H. Liu * and N. Behdad Department
More informationYour RF Cable, the unknown Entity
HAM RADIO 2018 Your RF Cable, the unknown Entity PROF. DR. THOMAS BAIER E-mail: baier@hs-ulm.de DG8SAQ Hochschule Ulm University of Applied Sciences Prittwitzstrasse 10 89075 Ulm Thanks to: Dan Maguire
More informationECE 451 Advanced Microwave Measurements. Requirements of Physical Channels
ECE 451 Advanced Microwave Measurements Requirements of Physical Channels Jose E. Schutt-Aine Electrical & Computer Engineering University of Illinois jschutt@emlab.uiuc.edu ECE 451 Jose Schutt Aine 1
More informationEELE 3332 Electromagnetic II Chapter 11. Transmission Lines. Islamic University of Gaza Electrical Engineering Department Dr.
EEE 333 Electromagnetic II Chapter 11 Transmission ines Islamic University of Gaza Electrical Engineering Department Dr. Talal Skaik 1 1 11.1 Introduction Wave propagation in unbounded media is used in
More informationExternal high-quality-factor resonator tunes up nuclear magnetic resonance
External high-quality-factor resonator tunes up nuclear magnetic resonance Stephan Appelt 1,*, Martin Suefke 3, Alexander Liebisch, and Bernhard Blümich 1 Central Institute for Engineering, Electronics
More information