InP HBT technology development at IEMN
|
|
- Godwin Hubbard
- 6 years ago
- Views:
Transcription
1 InP HBT technology development at IEMN Advanced NanOmetric Devices Group, Institut d Electronique de Microelectronique et de Nanotechnology, Lille, FRANCE Date
2 Outline Which applications for THz GaAsSb/InP DHBT GaInAs/InP SHBT Thermal Management 6.1 Å AlInAsSb/GaInSb DHBT Conclusion
3 Where is the Terahertz? mm Waves Submm Waves
4 Applications for Terahertz : Radio Astronomy Observation of the Universe Planck space telescope Cosmic Microwave Background Crédits : European Space Agency
5 Applications for Terahertz : Science Spectroscopy & Imaging Security Medical diagnostic Analysis
6 Applications for Terahertz : Telecommunication Optical Fiber Transmission 1 Gb/s 16 Gb/s Terahertz Wireless Communication High-Speed Wireless Transmission THz Carrier Frequency (.2,.6 THz) Data Rate : 4, 1 Gbit/s
7 Bande interdite (ev) FET &TBH 1 st generation Compound Semiductors for THz Devices FET &TBH 2 sd generation FET &TBH 3 th generation 2,5 2 GaP AlP AlAs AlSb Band Gap Engineering Versatility 1,5 1 GaAs InP ² GaSb AlInAs GaInAs InP GaAsSb GaSb AlSb InSb,5 InSb InAs InAs 5,4 5,5 5,6 5,7 5,8 5,9 6 6,1 6,2 6,3 6,4 6,5 Type I Type II Type III Type I Paramètre de maille (Å) Matériaux µ n (cm 2 /V.s) µ p (cm 2 /V.s) GaAs 85 4 InGaAs 11 3 InAs GaSb 5 85 AlSb 2 42 InSb Diverses Mobilities High Electron Mobility : InGaAs, InAs, InSb High Hole Mobility : GaSb, InSb
8 R E r E C BE III-V Bipolar Transistor : 3 Axes of Optimization 1 W E /2 = τ + τ + C r + C r + R base collector be E bc E 2πf Emitter Width InGaAs SG E InP Emitter Undercut v R Bint R Blink R Bext T r b c E C T T 2 b c nkt qi f = f 8πR E max / 2D / 2v n sat cb Ac /Tc ( ) τ ex + bb R C coll cbc Vertical Scaling : Epitaxy Lateral Scaling : Technology C BC Int C BC Link W BC /2 C BC Con Base-Collecteur Width R / R ex bb sh,e c, emet A We Wbc Wlink sh,bc sh,link 12L 6L 2L A e emet Ohmic Contacts Technology & Epitaxy e e contact contacts
9 Emitter Base Collector
10 Emitter Last Generation Base Emitter Dimension 15 2 nm Base Collector 1
11 InP DHBT Type-II Heterostruture InP/GaAsSb/InP Emitter n Base p Type II DHBT InP/GaAsSb : Interests & Structure Collector n Thickness (Å) Material Doping (cm -3 ) Description 5 In,85 Ga,15 As > : Si Emitter Cap 1 In x Ga 1-x As : Si Emit. Cap Grad. 8 InP : Si Emitter 35 InP : Si Emitter E c : C 3 GaAs 51 Sb 49 Base 13 Ω/o 13 InP : Si Collector E V Epitaxial Design Collector Potential Energy Injection High Confinement for Holes High Breakdown Voltage 1 InP : Si Sub-Collector 5 In,53 Ga,47 As : Si Cont. Sub-Coll. 2 InP : Si Sub-Collector 2 In,53 Ga,47 As NID Etch stop Substrate Semi-insulating InP
12 I C (ma/µm 2 ) I B, I C (A) Current Gain, Type II DHBT InP/GaAsSb : Results DC Measurements I B From to 8 µa 5 µa/step A E =.55 x 3.5 µm V CE (V) I B A E =.55 x 3.5 µm I C V CB = V 1-4 Gain V BE (V) BV CEO = 4.6 J E = 1 ka/cm 2 β = 24 M. Zaknoune, et al. IEEE EDL, Vol. 35, No. 3, 214. ρ CBase 7 Ω µm 2, Base ρ sheet = 13 Ω/ ρ CEmit. 2 Ω µm 2
13 Gain (db) Output Power (dbm), Power Gain (db) PAE (%) Results Type II DHBT InP/GaAsSb : RF & Power Measurements at 94 GHz V CE = 1.9 V I C = 6.7 ma/µm2 H 21 2 F T = 31 GHz U F MAX = 48 GHz F T = 31 GHz Frequency (Hz) F MAX = 48 GHz M. Zaknoune, et al. IEEE EDL, Vol. 35, No. 3, 214. A E =.55 x 3.5 µm Output Power (dbm) 12 Power Gain (db) 3 1 PAE (%) A E =.2 x 9.5 µm Absorbed Power (dbm) I C = 16 ma/µm 2, I B = 2.6 ma, V CE = 2.8 V P OUT = 12.8 dbm (1.26 mw/µm 2 ) P.A.E = 25 %, Power Gain = 4.5 db
14 Type I SHBT InP/InGaAs : Interets & Structrure InP SHBT Type-I Heterostruture InP/InGaAs/InGaAs Emitter n Base p Collector n Thickness (Å) Material Doping (cm -3 ) Description 5 InAs > : Si Emitter Cap 1 In x Ga 1-x As : Si Emit. Cap Grad. 7 InP : Si Emitter 3 InP : Si Emitter 3 In x Ga 1-x As : C Base Grad. Mature Epitaxial System High Electron Mobilty Low Breakdown Voltage E c E V 5 In x Ga 1-x As NID Collector Grad. In,53 Ga,47 As : Si Pulse Doping 1 In,53 Ga,47 As NID Collector 1 In,53 Ga,47 As : Si Sub-Collector 2 InP : Si Sub-Collector 5 In,53 Ga,47 As : Si Cont. Sub-Coll. 3 InP : Si Sub-Collector 2 In,53 Ga,47 As NID Etch stop Substrate Semi-insulating InP
15 I C (ma/µm 2 ) I C, I B (A) Current Gain, Type I SHBT InP/InGaAs : Results DC Measurements I B From to 7 µa 5 µa/step A E =.2 x 2.5 µm V CE (V).1 1E-3 1E-4 1E-5 1E-6 1E-7 1E-8 I B (A) A E =.2 x 2.5 µm 2 I C (A) V CB = V Beta 1E V BE BV CEO = 2.5 J E = 1 ka/cm 2 β = 12 ρ CBase 2 Ω µm 2, Base ρ sheet = 75Ω/ ρ CEmit. 2 Ω µm 2
16 Gain (db) (GHz) - Single Pole Extraction Output Power (dbm), Power Gain (db) Results V CE = 1.5 V I C = 5.8 ma/µm 2 A E =.2 x 2.5 µm 2 H21 2 U F T F T = 35 GHz F MAX = 63 GHz Type I SHBT InP/InGaAs : RF & Power Measurements at 94 GHz Single Pole Extraction Frequency (Hz) FT Output Power Power Gain PAE A E =.2 x 9.5 µm Absorbed Power (dbm) PAE (%) F T = 35 GHz F MAX = 63 GHz IEEE EDL Under review I C = 8 ma/µm 2, V CE = 2 V, I B = 2.5 ma P OUT = 12.1 dbm (8.6 mw/µm 2 ) P.A.E = 31 %, Power Gain = 6.3 db
17 F MAX (GHz HBT : State of the Art Teledyne DHBT UCSB DHBT UIUC SHBT UIUC DHBT ETHZ DHBT GaAsSb HRL DHBT Northrop DHBT NTT DHBT IEMN SHBT IEMN DHBT GaAsSb F T (GHz) 17
18 (W/Km) DHBT Thermal Management : Thermal Issues 1 at 3 K 8 InP Si (168) AlN (2) 6 4 InAs GaAs 2 InGaAs InAlAsInGaP SiN SiO polyimid Material High Dissipated Power High Junction Temperature Degraded Material Properties Poor Device Reliability and Low Median-Time-To-Failure (MTTF)
19 Bonding layer Inverse active structure Original Substrate Bonding layer Host substrate DHBT Thermal Management : Active Layer Transfer Principle Original substrate Inverse active structure Bonding layer Host substrate Pressure + Temperature Inverse active structure Bonding layer Host substrate E contact Emitter Thermocompression Au Au Au (host Sub) / Au ( active sub) Base Collector Bonding layer Host substrate FINAL STRUCTURE
20 Bonding layer Inverse active structure Original Substrate Bonding layer Host substrate DHBT Thermal Management : Active Layer Transfer Principle FINAL STRUCTURE Original substrate Inverse active structure Pressure + Temperature Thickness (Å) Material Doping (cm -3 ) Description Bonding layer 1 InP Host substrate : Si Collector 2 GaAs.51 Sb : C Base 2 Al x In 1-x P : Si Emitter 1 InP : Si Emitter Con. 2 In,53 Ga,47 As : Si Emit. Cap. E contact Substrate Emitter Base Collector Bonding layer Host substrate Inverse active structure Bonding layer Host substrate Thermocompression Au Au Au (host Sub) / Au ( active sub) Semi-insulating InP
21 DHBT Thermal Management : Host Substrate Ceramic Substrate of AlN Very High Roughness Non Effective Bonding Perfect Bonding On Si Substrate
22 DHBT Thermal Management : Active Layer Transfer Process HR Si Mo/Pt/Au : 25/4/25 Å Active Layer Ti/Au : 25/25 HR Silicon Host Substrate Low R TH : 1625 K/W Own InP Substrate R TH : 4452 K/W 65% Lower for Reported Device A. Thiam, et al. IEEE EDL, Vol. 35, no. 1, 214.
23 Bande interdite (ev) " 6.1 Å " Antimonide HBT : Ideal Structure? ΔEc =.7 ev 2,5 AlP.86 ev.35 ev.35 ev 2 1,5 1 GaP AlAs GaAs InP AlInAsSb AlSb ΔEv =.2 ev ΔEc =.57 ev 1.17 ev.44 ev.44 ev ΔEv =.16 ev Al.5 In.5 Sb,5 5,4 5,5 5,6 5,7 5,8 5,9 6 6,1 6,2 6,3 6,4 6,5 InAs Paramètre de maille (Å) GaSb Ga.65 In.35 Sb InSb Ga.5 In.5 Sb 23
24 " 6.1 Å" Antimonide HBT Type-II Heterostruture AlInAsSb/GaInSb/AlInAsSb Emitter n Base p " 6.1 Å " Antimonide HBT : AlInAsSb/GaInSb/AlInAsSb Collector n Thickness (Å) Material Doping (cm -3 ) Description 4 Ga,65 In,35 Sb : Te Emitter Cap 4 AlInAsSb : Te Emitter : C 4 Ga,51 In,49 Sb Base 7 Ω/o E c 15 AlInAsSb : Si Collector 3 Ga,5 In,5 Sb : Si Cont. Sub-Coll. 2 Metamorphic Buffer Substrate Semi-insulating InP E V High Electron Mobility High Hole Mobility Breakdown Voltage 24
25 metal metal oxydes " Ex Nihilo " Realization 6.1 Å HBT : semiconductor semiconductor Tunnel Effect Φ B Emitter Definition : AlInSb/GaInSb Wet Etching Selectivity Selectivity AlInSb/GaInSb HCl based solution S = 1 Selectivity GaInSb/AlInSb C 4 H 6 O 6 Tartric acid solution S = 12 Ohmic Contact : Doping Level Surface Treatment UV Ozone, NH 4 S, Ion Cleaning Interface Metal Mo, Ti, Pd
26 " Ex Nihilo " Realization 6.1 Å HBT : Al,33 In,67 As,31 Sb,69 /GaInSb/Al,33 In,67 As,31 Sb,69 TBH Emitter Width = 1 µm, Emitter Long = 5 µm After Air-Bridge Fabrication
27 I B, I C (A) Current Gain, Gain (db) I C (ma) A E = 2x15 m I B (A) I C (A) Beta AlInAsSb/GaInSb/AlInAsSb DHBT : DC and RF Performances V CE (V) A E = 2 x 15 µm 2 V CB = V I B From to 1 ma 1 µa/step V BE (V) V CE = 1.1 V I C = 2.65 ma/µm 2 H 21 2 F T = 52 GHz U F MAX = 49 GHz Frequency (Hz) A E = 1 x 15 µm 2 Current Density > 2 ka/cm 2 Current Gain = 2 RF Performances ~ 5 GHz E. Mairiaux, et al. IEEE EDL, Vol. 31, no. 4, 21.
28 I B, I C (A) Current Gain, Gain (db) I C (ma) A E = 2x15 m I B (A) I C (A) Beta AlInAsSb/GaInSb/AlInAsSb DHBT : DC and RF Performances V CE (V) A E = 2 x 15 µm 2 V CB = V I B From to 1 ma 1 µa/step V BE (V) V CE = 1.1 V I C = 2.65 ma/µm 2 H 21 2 F T = 52 GHz U F MAX = 49 GHz Frequency (Hz) A E = 1 x 15 µm 2 First World High frequency Demonstration F T = 52 GHz F MAX = 49 GHz Current Density > 2 ka/cm 2 Current Gain = 2 RF Performances ~ 5 GHz E. Mairiaux, et al. IEEE EDL, Vol. 31, no. 4, 21.
29 Conclusion GaAsSb/InP : High Output Level at 94 GHz GaAsSb/InP : High Output Level at 94 GHz Drastic Reduction of the Thermal Resistance when Active is Transferred on HR-Si Substrate 6.1 Å : First RF Demonstration at IEMN
DC Analysis of InP/GaAsSb DHBT Device Er. Ankit Sharma 1, Dr. Sukhwinder Singh 2
IOSR Journal of Electronics and Communication Engineering (IOSR-JECE) e-issn: 2278-2834,p- ISSN: 2278-8735.Volume 10, Issue 5, Ver. I (Sep - Oct.2015), PP 48-52 www.iosrjournals.org DC Analysis of InP/GaAsSb
More informationIndium Phosphide and Related Materials Selectively implanted subcollector DHBTs
Indium Phosphide and Related Materials - 2006 Selectively implanted subcollector DHBTs Navin Parthasarathy, Z. Griffith, C. Kadow, U. Singisetti, and M.J.W. Rodwell Dept. of Electrical and Computer Engineering,
More informationAC Analysis of InP/GaAsSb DHBT Device 1 Er. Ankit Sharma, 2 Dr. Sukhwinder Singh 1
American International Journal of Research in Science, Technology, Engineering & Mathematics Available online at http://www.iasir.net ISSN (Print): 2328-3491, ISSN (Online): 2328-3580, ISSN (CD-ROM): 2328-3629
More information100+ GHz Transistor Electronics: Present and Projected Capabilities
21 IEEE International Topical Meeting on Microwave Photonics, October 5-6, 21, Montreal 1+ GHz Transistor Electronics: Present and Projected Capabilities Mark Rodwell University of California, Santa Barbara
More informationFrequency Limits of Bipolar Integrated Circuits
IEEE MTT-S Symposium, June 13, 2006 Frequency Limits of Bipolar Integrated Circuits Mark Rodwell University of California, Santa Barbara Collaborators Z. Griffith, E. Lind, V. Paidi, N. Parthasarathy,
More informationHigh-Frequency Transistors High-Frequency ICs. Technologies & Applications
High-Frequency Transistors High-Frequency ICs Technologies & Applications Mark Rodwell University of California, Santa Barbara rodwell@ece.ucsb.edu 805-893-3244, 805-893-2362 fax Report Documentation Page
More informationHigh Power Performance InP/InGaAs Single HBTs
High Power Performance InP/InGaAs Single HBTs D Sawdai, K Hong, A Samelis, and D Pavlidis Solid-State Electronics Laboratory, Department of Electrical Engineering and Computer Science, The University of
More informationHIGH-SPEED TYPE-II GaAsSb/InP DHBTs FOR MIXED-SIGNAL IC APPLICATIONS HUIMING XU DISSERTATION
HIGH-SPEED TYPE-II GaAsSb/InP DHBTs FOR MIXED-SIGNAL IC APPLICATIONS BY HUIMING XU DISSERTATION Submitted in partial fulfillment of the requirements for the degree of Doctor of Philosophy in Electrical
More informationEquivalent circuit modeling of InP/InGaAs Heterojunction Phototransistor for application of Radio-on-fiber systems
Equivalent circuit modeling of InP/InGaAs Heterojunction Phototransistor for application of Radio-on-fiber systems Jae-Young Kim The Graduate School Yonsei University Department of Electrical and Electronic
More informationTHz Indium Phosphide Bipolar Transistor Technology
IEEE Compound Semiconductor IC Symposium, October 4-7, La Jolla, California THz Indium Phosphide Bipolar Transistor Technology Mark Rodwell University of California, Santa Barbara Coauthors: J. Rode, H.W.
More information30% PAE W-band InP Power Amplifiers using Sub-quarter-wavelength Baluns for Series-connected Power-combining
2013 IEEE Compound Semiconductor IC Symposium, October 13-15, Monterey, C 30% PAE W-band InP Power Amplifiers using Sub-quarter-wavelength Baluns for Series-connected Power-combining 1 H.C. Park, 1 S.
More informationDevice Research Conference 2007
Devie Researh Conerene 2007 560 GHz t, max InGaAs/InP DHBT in a novel dry-ethed emitter proess Erik Lind, Adam M. Crook, Zah Griith, and Mark J.W. Rodwell Department o Eletrial and Computer Engineering
More informationDEFENSE TECHNICAL INFORMATION CENTER
DEFENSE TECHNICAL INFORMATION CENTER [nformiiioitforthe Deffrtse Couutauuty Month Day Year DTI'C has determined on LL j that this Technical Document has the Distribution Statement checked below. The current
More informationHOT ELECTRON INJECTION EFFECT AND IMPROVED LINEARITY IN TYPE-I/II DHBT FOR MILLIMETER-WAVE MIXED SIGNAL CIRCUIT APPLICATIONS KUANG-YU CHENG
HOT ELECTRON INJECTION EFFECT AND IMPROVED LINEARITY IN TYPE-I/II DHBT FOR MILLIMETER-WAVE MIXED SIGNAL CIRCUIT APPLICATIONS BY KUANG-YU CHENG DISSERTATION Submitted in partial fulfillment of the requirements
More informationGalileo, Elephants, & Fast Nano-Devices
Presentation to NNIN REU interns, July 29, 2008 Galileo, Elephants, & Fast Nano-Devices Mark Rodwell University of California, Santa Barbara rodwell@ece.ucsb.edu 805-893-3244, 805-893-5705 fax Scaling:
More informationAlternative Channel Materials for MOSFET Scaling Below 10nm
Alternative Channel Materials for MOSFET Scaling Below 10nm Doug Barlage Electrical Requirements of Channel Mark Johnson Challenges With Material Synthesis Introduction Outline Challenges with scaling
More informationPhotovoltaic Cells for Optical Power and Data Transmission
Photovoltaic Cells for Optical Power and Transmission H. Helmers, S.P. Philipps, S.K. Reichmuth, E. Oliva, D. Lackner, A.W. Bett Fraunhofer Institute for Solar Energy Systems ISE European Telemetry and
More informationRecord I on (0.50 ma/μm at V DD = 0.5 V and I off = 100 na/μm) 25 nm-gate-length ZrO 2 /InAs/InAlAs MOSFETs
Record I on (0.50 ma/μm at V DD = 0.5 V and I off = 100 na/μm) 25 nm-gate-length ZrO 2 /InAs/InAlAs MOSFETs Sanghoon Lee 1*, V. Chobpattana 2,C.-Y. Huang 1, B. J. Thibeault 1, W. Mitchell 1, S. Stemmer
More informationRecord Extrinsic Transconductance (2.45 ms/μm at V DS = 0.5 V) InAs/In 0.53 Ga 0.47 As Channel MOSFETs Using MOCVD Source-Drain Regrowth
Record Extrinsic Transconductance (2.45 ms/μm at = 0.5 V) InAs/In 0.53 Ga 7 As Channel MOSFETs Using MOCVD Source-Drain Regrowth Sanghoon Lee 1*, C.-Y. Huang 1, A. D. Carter 1, D. C. Elias 1, J. J. M.
More informationSemiconductor Materials for Power Electronics (SEMPEL) GaN power electronics materials
Semiconductor Materials for Power Electronics (SEMPEL) GaN power electronics materials Kjeld Pedersen Department of Physics and Nanotechnology, AAU SEMPEL Semiconductor Materials for Power Electronics
More informationThin film PV Technologies III- V PV Technology
Thin film PV Technologies III- V PV Technology Week 5.1 Arno Smets ` (Source: NASA) III V PV Technology Semiconductor Materials III- V semiconductors: GaAs: GaP: InP: InAs: GaInAs: GaInP: AlGaInAs: AlGaInP:
More informationUp to 6 GHz Low Noise Silicon Bipolar Transistor Chip. Technical Data AT-41400
Up to 6 GHz Low Noise Silicon Bipolar Transistor Chip Technical Data AT-1 Features Low Noise Figure: 1.6 db Typical at 3. db Typical at. GHz High Associated Gain: 1.5 db Typical at 1.5 db Typical at. GHz
More informationRecent ETHZ-YEBES Developments in Low-Noise phemts for Cryogenic Amplifiers
Receivers & Array Workshop 2010 September 20th, 2010 Recent ETHZ-YEBES Developments in Low-Noise phemts for Cryogenic Amplifiers Andreas R. Alt, Colombo R. Bolognesi Millimeter-Wave Electronics Group (MWE)
More informationMSE 410/ECE 340: Electrical Properties of Materials Fall 2016 Micron School of Materials Science and Engineering Boise State University
MSE 410/ECE 340: Electrical Properties of Materials Fall 2016 Micron School of Materials Science and Engineering Boise State University Practice Final Exam 1 Read the questions carefully Label all figures
More informationGallium nitride futures and other stories
Dr Mike Cooke Gallium nitride-based devices look set to have increasingly wide application, at least if the contributions at December s International Electron Devices Meeting () in Washington DC are anything
More informationSub 300 nm Wavelength III-Nitride Tunnel-Injected Ultraviolet LEDs
Sub 300 nm Wavelength III-Nitride Tunnel-Injected Ultraviolet LEDs Yuewei Zhang, Sriram Krishnamoorthy, Fatih Akyol, Sadia Monika Siddharth Rajan ECE, The Ohio State University Andrew Allerman, Michael
More informationLecture 18: Photodetectors
Lecture 18: Photodetectors Contents 1 Introduction 1 2 Photodetector principle 2 3 Photoconductor 4 4 Photodiodes 6 4.1 Heterojunction photodiode.................... 8 4.2 Metal-semiconductor photodiode................
More informationEnhanced Emitter Transit Time for Heterojunction Bipolar Transistors (HBT)
Advances in Electrical Engineering Systems (AEES)` 196 Vol. 1, No. 4, 2013, ISSN 2167-633X Copyright World Science Publisher, United States www.worldsciencepublisher.org Enhanced Emitter Transit Time for
More informationFabrication of High-Speed Resonant Cavity Enhanced Schottky Photodiodes
Fabrication of High-Speed Resonant Cavity Enhanced Schottky Photodiodes Abstract We report the fabrication and testing of a GaAs-based high-speed resonant cavity enhanced (RCE) Schottky photodiode. The
More informationsub-mm-wave ICs, University of California, Santa Barbara
20th Annual Workshop on Interconnections within High Speed Digital Systems, Santa Fe, New Mexico, 3 6 May 2009 THz Transistors, sub-mm-wave ICs, mm-wave Systems Mark Rodwell University of California, Santa
More informationSub-mm-Wave Technologies: Systems, ICs, THz Transistors
2013 Asia-Pacific Microwave Conference, November 8th, Seoul Sub-mm-Wave Technologies: Systems, ICs, THz Transistors Mark Rodwell University of California, Santa Barbara Coauthors: J. Rode, H.W. Chiang,
More informationAn Overview of InP/GaAsSb/InP DHBT in Millimeter and Sub-millimeter Range
An Overview of InP/GaAsSb/InP DHBT in Millimeter and Sub-millimeter Range 1 Er. Ankit Sharma, 2 Dr. Sukhwinder Singh 1 Research Scholar PEC University Of Technology, Chandigarh INDIA 2 Supervisor, Assistant
More informationSEMICONDUCTOR ELECTRONICS: MATERIALS, DEVICES AND SIMPLE CIRCUITS. Class XII : PHYSICS WORKSHEET
SEMICONDUCT ELECTRONICS: MATERIALS, DEVICES AND SIMPLE CIRCUITS Class XII : PHYSICS WKSHEET 1. How is a n-p-n transistor represented symbolically? (1) 2. How does conductivity of a semiconductor change
More informationGallium nitride (GaN)
80 Technology focus: GaN power electronics Vertical, CMOS and dual-gate approaches to gallium nitride power electronics US research company HRL Laboratories has published a number of papers concerning
More informationEE 5611 Introduction to Microelectronic Technologies Fall Thursday, September 04, 2014 Lecture 02
EE 5611 Introduction to Microelectronic Technologies Fall 2014 Thursday, September 04, 2014 Lecture 02 1 Lecture Outline Review on semiconductor materials Review on microelectronic devices Example of microelectronic
More informationChapter 1. Introduction
Chapter 1 Introduction 1.1 Introduction of Device Technology Digital wireless communication system has become more and more popular in recent years due to its capability for both voice and data communication.
More informationDepartment of Electrical Engineering IIT Madras
Department of Electrical Engineering IIT Madras Sample Questions on Semiconductor Devices EE3 applicants who are interested to pursue their research in microelectronics devices area (fabrication and/or
More informationGeneral look back at MESFET processing. General principles of heterostructure use in FETs
SMA5111 - Compound Semiconductors Lecture 11 - Heterojunction FETs - General HJFETs, HFETs Last items from Lec. 10 Depletion mode vs enhancement mode logic Complementary FET logic (none exists, or is likely
More informationTransistor & IC design for Sub-mm-Wave & THz ICs
Plenary, 2012 European Microwave Integrated Circuits Conference, October 29th, Amsterdam Transistor & IC design for Sub-mm-Wave & THz ICs Mark Rodwell University of California, Santa Barbara Coauthors:
More informationLecture 24: Bipolar Junction Transistors (1) Bipolar Junction Structure, Operating Regions, Biasing
Lecture 24: Bipolar Junction Transistors (1) Bipolar Junction Structure, Operating Regions, Biasing BJT Structure the BJT is formed by doping three semiconductor regions (emitter, base, and collector)
More informationHigh performance InP/InAlAs/GaAsSb/InP double heterojunction bipolar transistors
Solid-State Electronics 5 (26) 92 97 www.elsevier.com/locate/sse High performance InP/InAlAs/GaAsSb/InP double heterojunction bipolar transistors S.W. Cho a, J.H. Yun a, D.H. Jun a, J.I. Song a, I. Adesida
More informationSupporting Information. Vertical Graphene-Base Hot-Electron Transistor
Supporting Information Vertical Graphene-Base Hot-Electron Transistor Caifu Zeng, Emil B. Song, Minsheng Wang, Sejoon Lee, Carlos M. Torres Jr., Jianshi Tang, Bruce H. Weiller, and Kang L. Wang Department
More informationLow Thermal Resistance Flip-Chip Bonding of 850nm 2-D VCSEL Arrays Capable of 10 Gbit/s/ch Operation
Low Thermal Resistance Flip-Chip Bonding of 85nm -D VCSEL Arrays Capable of 1 Gbit/s/ch Operation Hendrik Roscher In 3, our well established technology of flip-chip mounted -D 85 nm backside-emitting VCSEL
More informationtechniques, and gold metalization in the fabrication of this device.
Up to 6 GHz Medium Power Silicon Bipolar Transistor Chip Technical Data AT-42 Features High Output Power: 21. dbm Typical P 1 db at 2. GHz 2.5 dbm Typical P 1 db at 4. GHz High Gain at 1 db Compression:
More informationFiber-fed wireless systems based on remote up-conversion techniques
2008 Radio and Wireless Symposium incorporating WAMICON 22 24 January 2008, Orlando, FL. Fiber-fed wireless systems based on remote up-conversion techniques Jae-Young Kim and Woo-Young Choi Dept. of Electrical
More information50-500GHz Wireless Technologies: Transistors, ICs, and Systems
Plenary, Asia-Pacific Microwave Conference, December 6, 2015, Nanjing, China 50-500GHz Wireless Technologies: Transistors, ICs, and Systems Mark Rodwell, UCSB J. Rode*, P. Choudhary, B. Thibeault, W. Mitchell,
More informationarxiv:physics/ v2 [physics.optics] 17 Mar 2005
Optical modulation at around 1550 nm in a InGaAlAs optical waveguide containing a In- GaAs/AlAs resonant tunneling diode J. M. L. Figueiredo a), A. R. Boyd, C. R. Stanley, and C. N. Ironside Department
More informationSilicon Bipolar High f T Low Noise Medium Power 12 Volt Transistors
Silicon Bipolar High f T Low Noise Medium Power 1 Volt Transistors Features Low Phase Noise Oscillator Transistor mw Driver Amplifier Transistor Operation to GHz Available as Available in Hermetic Surface
More informationFrequency Limits of InP-based Integrated Circuits
Plenary, Indium Phosphide and Related Materials Conference, May 15-18, Matsue, Japan Frequency Limits of InP-based Integrated Circuits Mark Rodwell, E. Lind, Z. Griffith, S. R. Bank, A. M. Crook U. Singisetti,
More information2.8 - CMOS TECHNOLOGY
CMOS Technology (6/7/00) Page 1 2.8 - CMOS TECHNOLOGY INTRODUCTION Objective The objective of this presentation is: 1.) Illustrate the fabrication sequence for a typical MOS transistor 2.) Show the physical
More informationGaN MMIC PAs for MMW Applicaitons
GaN MMIC PAs for MMW Applicaitons Miroslav Micovic HRL Laboratories LLC, 311 Malibu Canyon Road, Malibu, CA 9265, U. S. A. mmicovic@hrl.com Motivation for High Frequency Power sources 6 GHz 11 GHz Frequency
More informationInstruction manual and data sheet ipca h
1/15 instruction manual ipca-21-05-1000-800-h Instruction manual and data sheet ipca-21-05-1000-800-h Broad area interdigital photoconductive THz antenna with microlens array and hyperhemispherical silicon
More informationChapter 3 Basics Semiconductor Devices and Processing
Chapter 3 Basics Semiconductor Devices and Processing 1 Objectives Identify at least two semiconductor materials from the periodic table of elements List n-type and p-type dopants Describe a diode and
More informationOptical Fiber Communication Lecture 11 Detectors
Optical Fiber Communication Lecture 11 Detectors Warriors of the Net Detector Technologies MSM (Metal Semiconductor Metal) PIN Layer Structure Semiinsulating GaAs Contact InGaAsP p 5x10 18 Absorption InGaAs
More informationDesign of InGaAs/InP 1.55μm vertical cavity surface emitting lasers (VCSEL)
Design of InGaAs/InP 1.55μm vertical cavity surface emitting lasers (VCSEL) J.-M. Lamy, S. Boyer-Richard, C. Levallois, C. Paranthoën, H. Folliot, N. Chevalier, A. Le Corre, S. Loualiche UMR FOTON 6082
More informationIntegrated diodes. The forward voltage drop only slightly depends on the forward current. ELEKTRONIKOS ĮTAISAI
1 Integrated diodes pn junctions of transistor structures can be used as integrated diodes. The choice of the junction is limited by the considerations of switching speed and breakdown voltage. The forward
More information3 Volt, Low Noise High ft Silicon Transistor. MP4T6310 Series. Features SOT-23. Description SOT-143. Chip
3 Volt, Low Noise High ft Silicon Transistor Features High Performance at VCE = 3V Low Noise Figure at Small Currents (.3- ma) High Gain (14 db) at 1mA Collector Current High ft (14 GHz) Available on Tape
More informationInnovative ultra-broadband ubiquitous Wireless communications through terahertz transceivers ibrow
Project Overview Innovative ultra-broadband ubiquitous Wireless communications through terahertz transceivers ibrow Mar-2017 Presentation outline Project key facts Motivation Project objectives Project
More informationNAME: Last First Signature
UNIVERSITY OF CALIFORNIA, BERKELEY College of Engineering Department of Electrical Engineering and Computer Sciences EE 130: IC Devices Spring 2003 FINAL EXAMINATION NAME: Last First Signature STUDENT
More informationFinal Report of 1.55 Vertical Cavity Surface Emitting Laser with Dielectric Mirrors
Final Report of 1.55 Vertical Cavity Surface Emitting Laser with Dielectric Mirrors Sponsored by: U. S. Army Research Office Dr. Michael D. Gerhold Contract Number: DAAD-19-01-1-0756 Submitted by Fan Ren
More informationData Sheet. AT Up to 6 GHz Medium Power Silicon Bipolar Transistor. Features. Description. 100 mil Package. High Output Power:
AT-1 Up to 6 GHz Medium Power Silicon Bipolar Transistor Data Sheet Description Avago s AT-1 is a general purpose NPN bipolar transistor that offers excellent high frequency performance. The AT-1 is housed
More information6.012 Microelectronic Devices and Circuits
Page 1 of 13 YOUR NAME Department of Electrical Engineering and Computer Science Massachusetts Institute of Technology 6.012 Microelectronic Devices and Circuits Final Eam Closed Book: Formula sheet provided;
More informationData Sheet. AT Up to 6 GHz Medium Power Silicon Bipolar Transistor. Description. Features. 85 Plastic Package
AT-85 Up to 6 GHz Medium Power Silicon Bipolar Transistor Data Sheet Description Avago s AT-85 is a general purpose NPN bipolar transistor that offers excellent high frequency performance. The AT-85 is
More informationCHAPTER I INTRODUCTION. mechanisms for the device are yet to be adequately understood. In this thesis, a detailed
CHAPTER I INTRODUCTION Indium Arsenide (InAs) channel high electron mobility transistors (HEMTs) with Aluminium Antimonide (AlSb) barriers are an exciting option for low power RF applications due to excellent
More informationA New SiGe Base Lateral PNM Schottky Collector. Bipolar Transistor on SOI for Non Saturating. VLSI Logic Design
A ew SiGe Base Lateral PM Schottky Collector Bipolar Transistor on SOI for on Saturating VLSI Logic Design Abstract A novel bipolar transistor structure, namely, SiGe base lateral PM Schottky collector
More informationWide Band-Gap Power Device
Wide Band-Gap Power Device 1 Contents Revisit silicon power MOSFETs Silicon limitation Silicon solution Wide Band-Gap material Characteristic of SiC Power Device Characteristic of GaN Power Device 2 1
More informationPower MOSFET Zheng Yang (ERF 3017,
ECE442 Power Semiconductor Devices and Integrated Circuits Power MOSFET Zheng Yang (ERF 3017, email: yangzhen@uic.edu) Evolution of low-voltage (
More informationIII-V CMOS: Quo Vadis?
III-V CMOS: Quo Vadis? J. A. del Alamo, X. Cai, W. Lu, A. Vardi, and X. Zhao Microsystems Technology Laboratories Massachusetts Institute of Technology Compound Semiconductor Week 2018 Cambridge, MA, May
More informationTU3B-1. An 81 GHz, 470 mw, 1.1 mm 2 InP HBT Power Amplifier with 4:1 Series Power Combining using Sub-quarter-wavelength Baluns
TU3B-1 Student Paper Finalist An 81 GHz, 470 mw, 1.1 mm 2 InP HBT Power Amplifier with 4:1 Series Power Combining using Sub-quarter-wavelength Baluns H. Park 1, S. Daneshgar 1, J. C. Rode 1, Z. Griffith
More informationMulti-GHz Operation of Tilted- Charge LED for Optical Interconnect
Multi-GHz Operation of Tilted- Charge LED for Optical Interconnect Chao-Hsin Wu 吳肇欣 Department of Electrical Engineering & Graduate Institute of Photonics and Optoelectronics & Graduate Institute of Electronics
More informationChapter 6. Silicon-Germanium Technologies
Chapter 6 licon-germanium Technologies 6.0 Introduction The design of bipolar transistors requires trade-offs between a number of parameters. To achieve a fast base transit time, hence achieving a high
More information32nm Technology and Beyond
32nm Technology and Beyond Paolo Gargini Chairman ITRS IEEE Fellow Director of Technology Strategy Intel Fellow ISS Europe 2009 P. Gargini 1 Agenda Equivalent Scaling 45nm Technology summary 32nm Technology
More informationPlanarization and Regrowth of Self-Aligned Ohmic Contacts on InGaAs
MBE 2008, Vancouver, B.C. Planarization and Regrowth of Self-Aligned Ohmic Contacts on InGaAs Mark Wistey, Greg Burek, Uttam Singisetti, Austin Nelson, Brian Thibeault, Joël Cagnon, Susanne Stemmer, Arthur
More informationHigh power and single frequency quantum. cascade lasers for gas sensing. Stéphane Blaser
High power and single frequency quantum cascade lasers for gas sensing Stéphane Blaser Alpes Lasers: Yargo Bonetti Lubos Hvozdara Antoine Muller University of Neuchâtel: Marcella Giovannini Nicolas Hoyler
More informationSemiconductor Lasers Semiconductors were originally pumped by lasers or e-beams First diode types developed in 1962: Create a pn junction in
Semiconductor Lasers Semiconductors were originally pumped by lasers or e-beams First diode types developed in 1962: Create a pn junction in semiconductor material Pumped now with high current density
More informationSilicon Bipolar Low Noise Microwave Transistors
Silicon Bipolar Low Noise Microwave Transistors MP42141 Features Case Styles Low Intrinsic Noise Figure (2.3dB Typical @ 1.0 GHz) High Power Gain At 1.0 GHz 18.0 db Typical Gold Metalization Hermetic and
More informationPHYSICAL ELECTRONICS(ECE3540) APPLICATIONS OF PHYSICAL ELECTRONICS PART I
PHYSICAL ELECTRONICS(ECE3540) APPLICATIONS OF PHYSICAL ELECTRONICS PART I Tennessee Technological University Monday, October 28, 2013 1 Introduction In the following slides, we will discuss the summary
More informationALMA MEMO 399 Millimeter Wave Generation Using a Uni-Traveling-Carrier Photodiode
ALMA MEMO 399 Millimeter Wave Generation Using a Uni-Traveling-Carrier Photodiode T. Noguchi, A. Ueda, H.Iwashita, S. Takano, Y. Sekimoto, M. Ishiguro, T. Ishibashi, H. Ito, and T. Nagatsuma Nobeyama Radio
More informationRF and Microwave Semiconductor Technologies
RF and Microwave Semiconductor Technologies Muhammad Fahim Ul Haque, Department of Electrical Engineering, Linköping University muhha@isy.liu.se Note: 1. This presentation is for the course of State of
More informationSingle-stage G-band HBT Amplifier with 6.3 db Gain at 175 GHz
Single-stage G-band HBT Amplifier with 6.3 db Gain at 175 GHz M. Urteaga, D. Scott, T. Mathew, S. Krishnan, Y. Wei, M.J.W. Rodwell Department of Electrical and Computer Engineering, University of California,
More informationUltra-low voltage resonant tunnelling diode electroabsorption modulator
Ultra-low voltage resonant tunnelling diode electroabsorption modulator, 1/10 Ultra-low voltage resonant tunnelling diode electroabsorption modulator J. M. L. FIGUEIREDO Faculdade de Ciências e Tecnologia,
More informationGallium Nitride & Related Wide Bandgap Materials and Devices
Gallium Nitride & Related Wide Bandgap Materials and Devices Dr. Edgar J. Martinez Program Manager DARPATech 2000 GaAs IC Markets 1999 Market $11 Billion 2005 Market $20 Billion Consumers 2% Computers
More informationRECENTLY, InP/GaAsSb/InP double heterojunction bipolar
IEEE TRANSACTIONS ON ELECTRON DEVICES, VOL. 57, NO. 12, DECEMBER 2010 3327 DC Characteristics of InAlAs/InGaAsSb/InGaAs Double Heterojunction Bipolar Transistors Shu-Han Chen, Member, IEEE, Chao-Min Chang,
More informationLong wavelength electrically pumped GaSb-based Buried Tunnel Junction VCSELs
Available online at www.sciencedirect.com Physics Physics Procedia Procedia 3 (2010) 00 (2009) 1155 1159 000 000 www.elsevier.com/locate/procedia 14 th International Conference on Narrow Gap Semiconductors
More informationGaN power electronics
GaN power electronics The MIT Faculty has made this article openly available. Please share how this access benefits you. Your story matters. Citation As Published Publisher Lu, Bin, Daniel Piedra, and
More informationChapter 3: Basics Semiconductor Devices and Processing 2006/9/27 1. Topics
Chapter 3: Basics Semiconductor Devices and Processing 2006/9/27 1 Topics What is semiconductor Basic semiconductor devices Basics of IC processing CMOS technologies 2006/9/27 2 1 What is Semiconductor
More informationUltra High-Speed InGaAs Nano-HEMTs
Ultra High-Speed InGaAs Nano-HEMTs 2003. 10. 14 Kwang-Seok Seo School of Electrical Eng. and Computer Sci. Seoul National Univ., Korea Contents Introduction to InGaAsNano-HEMTs Nano Patterning Process
More informationA STUDY INTO THE APPLICABILITY OF P + N + (UNIVERSAL CONTACT) TO POWER SEMICONDUCTOR DIODES AND TRANSISTORS FOR FASTER REVERSE RECOVERY
Thesis Title: Name: A STUDY INTO THE APPLICABILITY OF P + N + (UNIVERSAL CONTACT) TO POWER SEMICONDUCTOR DIODES AND TRANSISTORS FOR FASTER REVERSE RECOVERY RAGHUBIR SINGH ANAND Roll Number: 9410474 Thesis
More informationOptical Amplifiers. Continued. Photonic Network By Dr. M H Zaidi
Optical Amplifiers Continued EDFA Multi Stage Designs 1st Active Stage Co-pumped 2nd Active Stage Counter-pumped Input Signal Er 3+ Doped Fiber Er 3+ Doped Fiber Output Signal Optical Isolator Optical
More informationLecture Course. SS Module PY4P03. Dr. P. Stamenov
Semiconductor Devices - 2013 Lecture Course Part of SS Module PY4P03 Dr. P. Stamenov School of Physics and CRANN, Trinity College, Dublin 2, Ireland Hilary Term, TCD 01 st of Feb 13 Diode Current Components
More informationSolid State Device Fundamentals
Solid State Device Fundamentals 4.4. Field Effect Transistor (MOSFET) ENS 463 Lecture Course by Alexander M. Zaitsev alexander.zaitsev@csi.cuny.edu Tel: 718 982 2812 4N101b 1 Field-effect transistor (FET)
More informationUNIT-4. Microwave Engineering
UNIT-4 Microwave Engineering Microwave Solid State Devices Two problems with conventional transistors at higher frequencies are: 1. Stray capacitance and inductance. - remedy is interdigital design. 2.Transit
More informationX Band Driver Amplifier. GaAs Monolithic Microwave IC
GaAs Monolithic Microwave IC Description The CHA5012 chip is a monolithic twostage medium power amplifier designed for X band applications. This device is manufactured using a GaInP HBT process, including
More informationLecture 020 ECE4430 Review II (1/5/04) Page 020-1
Lecture 020 ECE4430 Review II (1/5/04) Page 020-1 LECTURE 020 ECE 4430 REVIEW II (READING: GHLM - Chap. 2) Objective The objective of this presentation is: 1.) Identify the prerequisite material as taught
More informationLecture 020 ECE4430 Review II (1/5/04) Page 020-1
Lecture 020 ECE4430 Review II (1/5/04) Page 020-1 LECTURE 020 ECE 4430 REVIEW II (READING: GHLM - Chap. 2) Objective The objective of this presentation is: 1.) Identify the prerequisite material as taught
More informationmhemt based MMICs, Modules, and Systems for mmwave Applications Axel Hülsmann Axel Tessmann Jutta Kühn Oliver Ambacher
mhemt based MMICs, Modules, and Systems for mmwave Applications Christaweg 54 79114 Freiburg, Germany +49 761 5951 4692 info@ondosense.com www.ondosense.com Axel Hülsmann Axel Tessmann Jutta Kühn Oliver
More informationCharacteristics of InP HEMT Harmonic Optoelectronic Mixers and Their Application to 60GHz Radio-on-Fiber Systems
. TU6D-1 Characteristics of Harmonic Optoelectronic Mixers and Their Application to 6GHz Radio-on-Fiber Systems Chang-Soon Choi 1, Hyo-Soon Kang 1, Dae-Hyun Kim 2, Kwang-Seok Seo 2 and Woo-Young Choi 1
More informationTHz communications: general issues THz devices for coms (Tx and Rx) Some Reported com links Some conclusions
THz communications for next generation HD rate wireless links TENXSYS Talk, 2015, June 17th G. Ducournau, M. Zaknoune, P. Szriftgiser, Jean-François Lampin (Tx and Rx) (Tx and Rx) 2 3 THz coms: general
More informationInP-based Complementary HBT Amplifiers for use in Communication Systems
InP-based Complementary HBT Amplifiers for use in Communication Systems Donald Sawdai and Dimitris Pavlidis Solid-State Electronics Laboratory Department of Electrical Engineering and Computer Science
More informationInnovative Technologies for RF & Power Applications
Innovative Technologies for RF & Power Applications > Munich > Nov 14, 2017 1 Key Technologies Key Technologies Veeco Market Focus Advanced Packaging, MEMS & RF Lighting, Display & Power Electronics Lithography
More information