Self-Aligned InGaAs FinFETs with 5-nm Fin-Width and 5-nm Gate-Contact Separation
|
|
- Tobias Young
- 6 years ago
- Views:
Transcription
1 Self-Aligned InGaAs FinFETs with 5-nm Fin-Width and 5-nm Gate-Contact Separation Alon Vardi, Lisa Kong, Wenjie Lu, Xiaowei Cai, Xin Zhao, Jesús Grajal* and Jesús A. del Alamo Microsystems Technology Laboratories, Massachusetts Institute of Technology, Cambridge, MA, U.S.A *ETSI Telecomunicación, Universidad Politécnica de Madrid, Madrid, Spain Dec. 5, 2017 Sponsors: DTRA (HDTRA ) NSF E3S STC (grant # ) Lam Research Korea Institute of Science and Technology 1
2 FinFETs Intel Si Trigate MOSFETs Double gate Tri gate FinFETs used in state of the art Si CMOS improved short channel effects smaller footprint but higher parasitics 2
3 Si and InGaAs FinFETs normalized by gate periphery [ms/ m] Si FinFETs 14 nm 22 nm Planar Si 32 nm // Planar Si planar FinFET: performance 3
4 Si and InGaAs FinFETs normalized by gate periphery normalized by fin footprint [ms/ m] Si FinFETs 14 nm 22 nm Planar Si 32 nm 0.0 // 0 // Planar Planar / [ms/ m] AR=H c / Si FinFETs (V DD =0.8 V) 4.3 Si planar FinFET: performance, performance per footprint Key challenge for FinFETs efficient transport on sidewalls H c 4
5 Si and InGaAs FinFETs normalized by gate periphery normalized by fin footprint [ms/ m] Si FinFETs 14 nm 22 nm 0.0 // 0 // Planar Planar III V planar ~ Si planar Planar InGaAs (V DD =0.5 V) Lin, EDL2016 Planar Si 32 nm / [ms/ m] AR=H c / Si FinFETs (V DD =0.8 V) 4.3 H c 5
6 Si and InGaAs FinFETs normalized by gate periphery normalized by fin footprint [ms/ m] Si FinFETs 14 nm 22 nm Planar InGaAs (V DD =0.5 V) Lin, EDL2016 Planar Si 32 nm 0.0 // 0 // Planar Planar / [ms/ m] (III V FinFETs) < (Si) Target of =5 nm yet to be demonstrated Target: W F =5 nm Si FinFETs (V DD =0.8 V) 4.3 InGaAs FinFETs H c 6
7 Si and InGaAs FinFETs normalized by gate periphery normalized by fin footprint [ms/ m] Si FinFETs 14 nm 22 nm Planar InGaAs (V DD =0.5 V) Lin, EDL2016 Planar Si 32 nm InGaAs FinFETs 0.0 // 0 // Planar Planar / [ms/ m] Target: W F =5 nm Si FinFETs (V DD =0.8 V) 4.3 III V FinFET: < 20 nm Challenge: Improve III V sidewall conductivity InGaAs FinFETs H c 7
8 SiO 2 Mo/W SiO 2 Mo/W cap Mo L f,g InGaAs channel Mo L g InGaAs channel InAlAs MIT InGaAs FinFET s Gen. #2 vs. #1 SiO 2 Mo/W InGaAs InAlAs Wet recess Gen. #1: Vardi et al., VLSI 2016, EDL nm Gen #2: L f HSQ SiO 2 HfO 2 Mo/W Cap Channel Dry+DE recess InP 40nm ~20 nm ~5 nm Gen #1: Wet cap recess 3 Digital etch cycles 40 nm channel height δ doping Dry cap recess 5 Digital etch cycles 50 nm channel Fin top passivation Remove δ doping (in 2 nd stage) Gen. #2: This work 8
9 Process Technology: contact-first W direction L g direction InP stopper Doping SiO 2 Mo/W InGaAs cap InGaAs channel InAlAs Contact deposition Yield R C < 10 Ω µm Lin, IEDM 2013 Lu, EDL 2014 Vardi, EDL
10 W direction Dry+Digital Etch cap recess L g direction InP stopper Doping Mo/W InGaAs cap InGaAs channel InAlAs Contact etch Reactive ion etching No metal pullback III V cap pullback only during digital etch L f L g Digital etching SiO 2 Mo/W Cap Channel Dry+DE recess 40nm ~5 nm (Lin, IEDM 2013) 10
11 Dry+Digital Etch fin definition direction HSQ H c Fin H f L g direction SiO 2 Mo/W L g cap InGaAs channel HSQ Zhao, EDL 2014, Vardi, VLSI nm 8 nm InAlAs Cap recess Fin etch fin 100 nm BCl 3 /SiCl 4 /Ar RIE + 5 DE cycles : smooth, vertical sidewalls and high aspect ratio (>10) 11
12 Gate stack - Double gate FinFET W direction HSQ Top fin passivation HfO 2 H f H c InP stopper L g direction SiO 2 Mo/W InGaAs cap InGaAs channel L g HSQ Mo Doping InAlAs Contact deposition Cap recess Fin etch Gate stack HSQ stays on top of fins double gate FinFET Gate oxide 3 nm HfO 2 (vs. 2.3 nm in EDL2016) fin 12
13 Device cross section TEM of finished device in direction FIB cross section in L g direction 5 nm Fin pitch: 200 nm fins/device : 5 25 nm L g : 30 nm 5 µm Contact to channel separation set by DE : ~5 nm 13
14 Electrical characteristics: =5 nm, L g =50 nm I d [ A/ m] V GS =-0.2 to 0.5 V V GS =0.1 V Normalized by gate periphery V GS [V] I d [A/ m] 1E-3 1E-4 1E-5 1E-6 1E-7 1E-8 1E-9 L g =50 nm =5 nm V DS =500 mv S sat =100 mv/dec S lin =73 mv/dec V GS [V] 50 mv [ S/ m] Well behaved devices with =5 nm V DS =0.5 V L g =50 nm =5 nm,max =600 µs/µm V GS [V] 14
15 On/Off performance: fin width scaling S sat [mv/dec] V DS = 0.5 V L g =40 60 nm [ms/ m] 2.0 V DS = 0.5 V L g =40 60 nm : S sat : 15
16 To improve Off performance: remove δ-doping Gen. #1 Gen. #2 δ doped SiO 2 Mo cap InGaAs Mo HSQ Gen. #2 Undoped SiO 2 Mo cap InGaAs Mo HSQ InAlAs Doping fin Extrinsic area δ doping R sd Dry gate recess allows to remove δ doping Impact on the intrinsic fin transport 16
17 W F =5 nm FinFET: Electrical characteristics: δ-doped vs. undoped I d [ A/ m] V GS =-0.2 to 0.5 V V GS =0.1 V Normalized by gate periphery V GS [V] I d [A/ m] 1E-3 1E-4 1E-5 1E-6 1E-7 1E-8 1E-9 Undoped fins: L g =50 nm =5 nm V DS =500 mv S sat =100 mv/dec S lin =73 mv/dec S sat =75 mv/dec S lin =65 mv/dec V GS [V] 50 mv [ S/ m] better OFF performance Undoped Similar ON performance V DS =0.5 V L g =50 nm =5 nm,max =600 µs/µm,max =500 µs/µm doped undoped V GS [V] 17
18 Electrical characteristics: δ-doped vs. undoped S sat [mv/dec] 180 Undoped -doped L g =40 60 nm [ms/ m] Undoped -doped V DS = 0.5 V L g =40 60 nm Undoped fin: improved electrostatics For <20 nm undoped fin ON performance also better 18
19 Electrical characteristics: V T rolloff Undoped δ doped V T,lin [V] W F L g V T,lin [V] =5 nm =9 =13 =17 =21 =25 W F L g Undoped fins smaller variation of V T with W F Improved V T rolloff 19
20 normalized by gate periphery Benchmarking H c H c [ms/ m] Undoped -doped Si FinFETs InGaAs FinFETs Systematic degradation for < 15 nm for both δ doped and undoped structures No improvement from increased #DE cycles Higher EOT lower w.r.t. to Gen. 1 20
21 H c H c [ms/ m] normalized by gate periphery Undoped -doped Si FinFETs Benchmarking InGaAs FinFETs / [ms/ m] Record with good electrical performance Approaching Si FinFETs even at V DD =0.5 V Record AR= Target: W F =5 nm Si FinFETs (V DD =0.8 V) 4.3 Undoped -doped InGaAs FinFETs
22 Long-channel Mobility vs. Capacitance 1GHz δ doped undoped =25 nm =9 nm Strong µ degradation as < 10 nm µ independent of n l 22
23 Simulations charge distribution =25 nm undoped ON state: n l =3x10 7 cm 1 δ doped y Undoped fin: better use of sidewalls δ doped fin: conduction close to lower facet of channel 23
24 Simulations charge distribution =25 nm ON state: n l =3x10 7 cm 1 undoped undoped =9 nm δ doped δ doped y Narrow fin: volume inversion in both δ doped and undoped fins 24
25 undoped Simulations capacitance =25 nm ON state: n l =3x10 7 cm 1 (V GT ~0.4V) undoped undoped =9 nm undoped δ doped Simulation δ doped δ doped δ doped Simulation E s (y) Simulation y Simulation Reasonable agreement between measurement and simulations extract n l E s relation 25
26 Simulations Mobility vs. Field δ doped undoped Body conductance δ doped undoped =25 nm =25 nm =9 nm =9 nm At similar n l : Wide fin: E S (δ doped) < E S (undoped) Narrow fin: E S (δ doped) ~ E S (undoped) 26
27 Long-channel Mobility vs n l = 3x10 7 cm 1 V GT ~ 0.4 V 1500 n l = 3x10 7 cm 1 V GT ~ 0.4 V [cm 2 /Vsec] δ doped -doped [cm 2 /Vsec] Undoped Undoped Large over drive: µ(δ doped) ~ µ(undoped) Strong µ degradation as < 10 nm µ saturate 27
28 Conclusions Self-aligned gate-last InGaAs FinFET: Self-aligned gate and contact trough precision RIE and digital etch Record AR=10 Record =5 nm InGaAs FinFET with good electrical performance Performance enhancement in narrow fins via δ-doping removal Thank you! 28
InGaAs Double-Gate Fin-Sidewall MOSFET
InGaAs Double-Gate Fin-Sidewall MOSFET Alon Vardi, Xin Zhao and Jesús del Alamo Microsystems Technology Laboratories, MIT June 25, 214 Sponsors: Sematech, Technion-MIT Fellowship, and NSF E3S Center (#939514)
More informationQuantum-size effects in sub-10 nm fin width InGaAs finfets
Quantum-size effects in sub-10 nm fin width InGaAs finfets Alon Vardi, Xin Zhao, and Jesús A. del Alamo Microsystems Technology Laboratories, MIT December 9, 2015 Sponsors: DTRA NSF (E3S STC) Northrop
More informationHigh aspect-ratio InGaAs FinFETs with sub-20 nm fin width
High aspect-rati InGaAs FinFETs with sub-2 nm fin width Aln Vardi, Jianqiang Lin, Wenjie Lu, Xin Zha and Jesús A. del Alam Micrsystems Technlgy Labratries, MIT June 15, 216 Spnsrs: DTRA (HDTRA 1-14-1-57),
More informationElectric-Field Induced F - Migration in Self-Aligned InGaAs MOSFETs and Mitigation
Electric-Field Induced F - Migration in Self-Aligned InGaAs MOSFETs and Mitigation X. Cai, J. Lin, D. A. Antoniadis and J. A. del Alamo Microsystems Technology Laboratories, MIT December 5, 2016 Sponsors:
More informationIII-V CMOS: What have we learned from HEMTs? J. A. del Alamo, D.-H. Kim 1, T.-W. Kim, D. Jin, and D. A. Antoniadis
III-V CMOS: What have we learned from HEMTs? J. A. del Alamo, D.-H. Kim 1, T.-W. Kim, D. Jin, and D. A. Antoniadis Microsystems Technology Laboratories, MIT 1 presently with Teledyne Scientific 23rd International
More informationPerformance Enhancement of P-channel InGaAs Quantum-well FETs by Superposition of Process-induced Uniaxial Strain and Epitaxially-grown Biaxial Strain
Performance Enhancement of P-channel InGaAs Quantum-well FETs by Superposition of Process-induced Uniaxial Strain and Epitaxially-grown Biaxial Strain Ling Xia 1, Vadim Tokranov 2, Serge R. Oktyabrsky
More informationThe Prospects for III-Vs
10 nm CMOS: The Prospects for III-Vs J. A. del Alamo, Dae-Hyun Kim 1, Donghyun Jin, and Taewoo Kim Microsystems Technology Laboratories, MIT 1 Presently with Teledyne Scientific 2010 European Materials
More information30 nm In 0.7 Ga 0.3 As Inverted-type HEMT with Reduced Gate Leakage Current for Logic Applications
30 nm In 0.7 Ga 0.3 As Inverted-type HEMT with Reduced Gate Leakage Current for Logic Applications T.-W. Kim, D.-H. Kim* and J. A. del Alamo Microsystems Technology Laboratories MIT Presently with Teledyne
More informationThe Pennsylvania State University. Kurt J. Lesker Company. North Carolina State University. Taiwan Semiconductor Manufacturing Company 1
Enhancement Mode Strained (1.3%) Germanium Quantum Well FinFET (W fin =20nm) with High Mobility (μ Hole =700 cm 2 /Vs), Low EOT (~0.7nm) on Bulk Silicon Substrate A. Agrawal 1, M. Barth 1, G. B. Rayner
More informationMicrosystems Technology Laboratories, MIT. Teledyne Scientific Company (TSC)
Extraction of Virtual-Source Injection Velocity in sub-100 nm III-V HFETs 1,2) D.-H. Kim, 1) J. A. del Alamo, 1) D. A. Antoniadis and 2) B. Brar 1) Microsystems Technology Laboratories, MIT 2) Teledyne
More informationUltra-Scaled InAs HEMTs
Performance Analysis of Ultra-Scaled InAs HEMTs Neerav Kharche 1, Gerhard Klimeck 1, Dae-Hyun Kim 2,3, Jesús. A. del Alamo 2, and Mathieu Luisier 1 1 Network for Computational ti Nanotechnology and Birck
More informationNegative-Bias Temperature Instability (NBTI) of GaN MOSFETs
Negative-Bias Temperature Instability (NBTI) of GaN MOSFETs Alex Guo and Jesús A. del Alamo Microsystems Technology Laboratories (MTL) Massachusetts Institute of Technology (MIT) Cambridge, MA, USA Sponsor:
More informationEE410 vs. Advanced CMOS Structures
EE410 vs. Advanced CMOS Structures Prof. Krishna S Department of Electrical Engineering S 1 EE410 CMOS Structure P + poly-si N + poly-si Al/Si alloy LPCVD PSG P + P + N + N + PMOS N-substrate NMOS P-well
More informationScaling Issues in Planar FET: Dual Gate FET and FinFETs
Scaling Issues in Planar FET: Dual Gate FET and FinFETs Lecture 12 Dr. Amr Bayoumi Fall 2014 Advanced Devices (EC760) Arab Academy for Science and Technology - Cairo 1 Outline Scaling Issues for Planar
More informationTechnology Development & Design for 22 nm InGaAs/InP-channel MOSFETs
2008 Indium Phosphide and Related Materials Conference, May, Versailles, France Technology Development & Design for 22 nm InGaAs/InP-channel MOSFETs M. Rodwell University of California, Santa Barbara M.
More informationEECS130 Integrated Circuit Devices
EECS130 Integrated Circuit Devices Professor Ali Javey 10/30/2007 MOSFETs Lecture 4 Reading: Chapter 17, 19 Announcements The next HW set is due on Thursday. Midterm 2 is next week!!!! Threshold and Subthreshold
More informationPerformance Analysis of Ultra-Scaled InAs HEMTs
Purdue University Purdue e-pubs Birck and NCN Publications Birck Nanotechnology Center 2009 Performance Analysis of Ultra-Scaled InAs HEMTs Neerav Kharche Birck Nanotechnology Center and Purdue University,
More informationElectrical Degradation of InAlAs/InGaAs Metamorphic High-Electron Mobility Transistors
Electrical Degradation of InAlAs/InGaAs Metamorphic High-Electron Mobility Transistors S. D. Mertens and J.A. del Alamo Massachusetts Institute of Technology Sponsor: Agilent Technologies Outline Introduction
More informationECE-305: Spring 2016 MOSFET IV
ECE-305: Spring 2016 MOSFET IV Professor Mark Lundstrom Electrical and Computer Engineering Purdue University, West Lafayette, IN USA lundstro@purdue.edu Lundstrom s lecture notes: Lecture 4 4/7/16 outline
More informationEE 560 MOS TRANSISTOR THEORY PART 2. Kenneth R. Laker, University of Pennsylvania
1 EE 560 MOS TRANSISTOR THEORY PART nmos TRANSISTOR IN LINEAR REGION V S = 0 V G > V T0 channel SiO V D = small 4 C GC C BC substrate depletion region or bulk B p nmos TRANSISTOR AT EDGE OF SATURATION
More informationRecent Development of FinFET Technology for CMOS Logic and Memory
Recent Development of FinFET Technology for CMOS Logic and Memory Chung-Hsun Lin EECS Department University of California at Berkeley Why FinFET Outline FinFET process Unique features of FinFET Mobility,
More information1464 IEEE TRANSACTIONS ON ELECTRON DEVICES, VOL. 63, NO. 4, APRIL 2016
1464 IEEE TRANSACTIONS ON ELECTRON DEVICES, VOL. 63, NO. 4, APRIL 2016 Analysis of Resistance and Mobility in InGaAs Quantum-Well MOSFETs From Ballistic to Diffusive Regimes Jianqiang Lin, Member, IEEE,
More informationReliability and Instability of GaN MIS-HEMTs for Power Electronics
Reliability and Instability of GaN MIS-HEMTs for Power Electronics Jesús A. del Alamo, Alex Guo and Shireen Warnock Microsystems Technology Laboratories Massachusetts Institute of Technology 2016 Fall
More informationCMPEN 411 VLSI Digital Circuits. Lecture 03: MOS Transistor
CMPEN 411 VLSI Digital Circuits Lecture 03: MOS Transistor Kyusun Choi [Adapted from Rabaey s Digital Integrated Circuits, Second Edition, 2003 J. Rabaey, A. Chandrakasan, B. Nikolic] CMPEN 411 L03 S.1
More informationComponents Research, TMG Intel Corporation *QinetiQ. Contact:
1 High-Performance 4nm Gate Length InSb P-Channel Compressively Strained Quantum Well Field Effect Transistors for Low-Power (V CC =.5V) Logic Applications M. Radosavljevic,, T. Ashley*, A. Andreev*, S.
More informationESE 570: Digital Integrated Circuits and VLSI Fundamentals
ESE 570: Digital Integrated Circuits and VLSI Fundamentals Lec 4: January 23, 2018 MOS Transistor Theory, MOS Model Penn ESE 570 Spring 2018 Khanna Lecture Outline! CMOS Process Enhancements! Semiconductor
More informationComparison of Ultra-Thin InAs and InGaAs Quantum Wells and Ultra-Thin-Body Surface-Channel MOSFETs
Comparison of Ultra-Thin InAs and InGaAs Quantum Wells and Ultra-Thin-Body Surface-Channel MOSFETs Cheng-Ying Huang 1, Sanghoon Lee 1, Evan Wilson 3, Pengyu Long 3, Michael Povolotskyi 3, Varistha Chobpattana
More informationThe Devices. Digital Integrated Circuits A Design Perspective. Jan M. Rabaey Anantha Chandrakasan Borivoje Nikolic. July 30, 2002
Digital Integrated Circuits A Design Perspective Jan M. Rabaey Anantha Chandrakasan Borivoje Nikolic The Devices July 30, 2002 Goal of this chapter Present intuitive understanding of device operation Introduction
More informationEnhanced Mobility CMOS
Enhanced Mobility CMOS Judy L. Hoyt I. Åberg, C. Ni Chléirigh, O. Olubuyide, J. Jung, S. Yu, E.A. Fitzgerald, and D.A. Antoniadis Microsystems Technology Laboratory MIT, Cambridge, MA 02139 Acknowledge
More informationTechnology Development for InGaAs/InP-channel MOSFETs
MRS Spring Symposium, Tutorial: Advanced CMOS Substrates, Devices, Reliability, and Characterization, April 13, 2009, San Francisco Technology Development for InGaAs/InP-channel MOSFETs Mark Rodwell University
More informationMOS Transistor Properties Review
MOS Transistor Properties Review 1 VLSI Chip Manufacturing Process Photolithography: transfer of mask patterns to the chip Diffusion or ion implantation: selective doping of Si substrate Oxidation: SiO
More informationEE115C Winter 2017 Digital Electronic Circuits. Lecture 3: MOS RC Model, CMOS Manufacturing
EE115C Winter 2017 Digital Electronic Circuits Lecture 3: MOS RC Model, CMOS Manufacturing Agenda MOS Transistor: RC Model (pp. 104-113) S R on D CMOS Manufacturing Process (pp. 36-46) S S C GS G G C GD
More informationAdvanced and Emerging Devices: SEMATECH s Perspective
SEMATECH Symposium October 23, 2012 Seoul Accelerating the next technology revolution Advanced and Emerging Devices: SEMATECH s Perspective Paul Kirsch Director, FEP Division Copyright 2012 SEMATECH, Inc.
More information! CMOS Process Enhancements. ! Semiconductor Physics. " Band gaps. " Field Effects. ! MOS Physics. " Cut-off. " Depletion.
ESE 570: Digital Integrated Circuits and VLSI Fundamentals Lec 4: January 3, 018 MOS Transistor Theory, MOS Model Lecture Outline! CMOS Process Enhancements! Semiconductor Physics " Band gaps " Field Effects!
More informationECE 305: Fall MOSFET Energy Bands
ECE 305: Fall 2016 MOSFET Energy Bands Professor Peter Bermel Electrical and Computer Engineering Purdue University, West Lafayette, IN USA pbermel@purdue.edu Pierret, Semiconductor Device Fundamentals
More informationALD high-k and higher-k integration on GaAs
ALD high-k and higher-k integration on GaAs Ozhan Koybasi 1), Min Xu 1), Yiqun Liu 2), Jun-Jieh Wang 2), Roy G. Gordon 2), and Peide D. Ye 1)* 1) School of Electrical and Computer Engineering, Purdue University,
More informationECE-305: Fall 2017 MOS Capacitors and Transistors
ECE-305: Fall 2017 MOS Capacitors and Transistors Pierret, Semiconductor Device Fundamentals (SDF) Chapters 15+16 (pp. 525-530, 563-599) Professor Peter Bermel Electrical and Computer Engineering Purdue
More informationAnomalous Source-side Degradation of InAlN/GaN HEMTs under ON-state Stress
Anomalous Source-side Degradation of InAlN/GaN HEMTs under ON-state Stress Yufei Wu, Jesús A. del Alamo Microsystems Technology Laboratories, Massachusetts Institute of Technology October 04, 2016 Sponsor:
More informationA Multi-Gate CMOS Compact Model BSIMMG
A Multi-Gate CMOS Compact Model BSIMMG Darsen Lu, Sriramkumar Venugopalan, Tanvir Morshed, Yogesh Singh Chauhan, Chung-Hsun Lin, Mohan Dunga, Ali Niknejad and Chenming Hu University of California, Berkeley
More informationTime Dependent Dielectric Breakdown in High Voltage GaN MIS HEMTs: The Role of Temperature
Time Dependent Dielectric Breakdown in High Voltage GaN MIS HEMTs: The Role of Temperature Shireen Warnock, Allison Lemus, and Jesús A. del Alamo Microsystems Technology Laboratories (MTL) Massachusetts
More informationVLSI Design and Simulation
VLSI Design and Simulation Performance Characterization Topics Performance Characterization Resistance Estimation Capacitance Estimation Inductance Estimation Performance Characterization Inverter Voltage
More informationESE 570: Digital Integrated Circuits and VLSI Fundamentals
ESE 570: Digital Integrated Circuits and VLSI Fundamentals Lec 4: January 29, 2019 MOS Transistor Theory, MOS Model Penn ESE 570 Spring 2019 Khanna Lecture Outline! CMOS Process Enhancements! Semiconductor
More informationPhysics-based compact model for ultimate FinFETs
Physics-based compact model for ultimate FinFETs Ashkhen YESAYAN, Nicolas CHEVILLON, Fabien PREGALDINY, Morgan MADEC, Christophe LALLEMENT, Jean-Michel SALLESE nicolas.chevillon@iness.c-strasbourg.fr Research
More informationHigh Mobility Materials and Novel Device Structures for High Performance Nanoscale MOSFETs
High Mobility Materials and Novel Device Structures for High Performance Nanoscale MOSFETs Prof. (Dr.) Tejas Krishnamohan Department of Electrical Engineering Stanford University, CA & Intel Corporation
More informationThe Devices. Digital Integrated Circuits A Design Perspective. Jan M. Rabaey Anantha Chandrakasan Borivoje Nikolic. July 30, 2002
igital Integrated Circuits A esign Perspective Jan M. Rabaey Anantha Chandrakasan Borivoje Nikolic The evices July 30, 2002 Goal of this chapter Present intuitive understanding of device operation Introduction
More informationMultiple Gate CMOS and Beyond
Multiple CMOS and Beyond Dept. of EECS, KAIST Yang-Kyu Choi Outline 1. Ultimate Scaling of MOSFETs - 3nm Nanowire FET - 8nm Non-Volatile Memory Device 2. Multiple Functions of MOSFETs 3. Summary 2 CMOS
More informationGraphene and new 2D materials: Opportunities for High Frequencies applications
Graphene and new 2D materials: Opportunities for High Frequencies applications April 21th, 2015 H. Happy, E. Pallecchi, B. Plaçais, D. Jiménez, R. Sordan, D. Neumaier Graphene Flagship WP4 HF electronic
More informationLecture 11: MOSFET Modeling
Digital Integrated Circuits (83-313) Lecture 11: MOSFET ing Semester B, 2016-17 Lecturer: Dr. Adam Teman TAs: Itamar Levi, Robert Giterman 18 June 2017 Disclaimer: This course was prepared, in its entirety,
More informationDigital Integrated Circuits A Design Perspective. Jan M. Rabaey Anantha Chandrakasan Borivoje Nikolic. The Devices. July 30, Devices.
Digital Integrated Circuits A Design Perspective Jan M. Rabaey Anantha Chandrakasan Borivoje Nikolic The July 30, 2002 1 Goal of this chapter Present intuitive understanding of device operation Introduction
More informationSupporting information
Supporting information Design, Modeling and Fabrication of CVD Grown MoS 2 Circuits with E-Mode FETs for Large-Area Electronics Lili Yu 1*, Dina El-Damak 1*, Ujwal Radhakrishna 1, Xi Ling 1, Ahmad Zubair
More information! CMOS Process Enhancements. ! Semiconductor Physics. " Band gaps. " Field Effects. ! MOS Physics. " Cut-off. " Depletion.
ESE 570: Digital Integrated Circuits and VLSI Fundamentals Lec 4: January 9, 019 MOS Transistor Theory, MOS Model Lecture Outline CMOS Process Enhancements Semiconductor Physics Band gaps Field Effects
More informationMOSFET: Introduction
E&CE 437 Integrated VLSI Systems MOS Transistor 1 of 30 MOSFET: Introduction Metal oxide semiconductor field effect transistor (MOSFET) or MOS is widely used for implementing digital designs Its major
More informationLow Frequency Noise in MoS 2 Negative Capacitance Field-effect Transistor
Low Frequency Noise in MoS Negative Capacitance Field-effect Transistor Sami Alghamdi, Mengwei Si, Lingming Yang, and Peide D. Ye* School of Electrical and Computer Engineering Purdue University West Lafayette,
More informationTri-Gate Fully-Depleted CMOS Transistors: Fabrication, Design and Layout
Tri-Gate Fully-Depleted CMOS Transistors: Fabrication, Design and Layout B.Doyle, J.Kavalieros, T. Linton, R.Rios B.Boyanov, S.Datta, M. Doczy, S.Hareland, B. Jin, R.Chau Logic Technology Development Intel
More informationScaling Effects on Single-Event Transients in InGaAs FinFETs
> REPLACE THIS LINE WITH YOUR PAPER IDENTIFICATION NUMBER (DOUBLE-CLICK HERE TO EDIT) < 1 Scaling Effects on Single-Event Transients in InGaAs FinFETs Huiqi Gong, Student Member, IEEE, Kai Ni, Student
More informationUltimately Scaled CMOS: DG FinFETs?
Ultimately Scaled CMOS: DG FinFETs? Jerry G. Fossum SOI Group Department of Electrical and Computer Engineering University of Florida Gainesville, FL 32611-6130 J. G. Fossum / 1 Outline Introduction -
More informationCHAPTER 5 EFFECT OF GATE ELECTRODE WORK FUNCTION VARIATION ON DC AND AC PARAMETERS IN CONVENTIONAL AND JUNCTIONLESS FINFETS
98 CHAPTER 5 EFFECT OF GATE ELECTRODE WORK FUNCTION VARIATION ON DC AND AC PARAMETERS IN CONVENTIONAL AND JUNCTIONLESS FINFETS In this chapter, the effect of gate electrode work function variation on DC
More informationOperation and Modeling of. The MOS Transistor. Second Edition. Yannis Tsividis Columbia University. New York Oxford OXFORD UNIVERSITY PRESS
Operation and Modeling of The MOS Transistor Second Edition Yannis Tsividis Columbia University New York Oxford OXFORD UNIVERSITY PRESS CONTENTS Chapter 1 l.l 1.2 1.3 1.4 1.5 1.6 1.7 Chapter 2 2.1 2.2
More informationOFF-state TDDB in High-Voltage GaN MIS-HEMTs
OFF-state TDDB in High-Voltage GaN MIS-HEMTs Shireen Warnock and Jesús A. del Alamo Microsystems Technology Laboratories (MTL) Massachusetts Institute of Technology (MIT) Purpose Further understanding
More informationSupporting Information for: Sustained sub-60 mv/decade switching via the negative capacitance effect in MoS 2 transistors
Supporting Information for: Sustained sub-60 mv/decade switching via the negative capacitance effect in MoS 2 transistors Felicia A. McGuire 1, Yuh-Chen Lin 1, Katherine Price 1, G. Bruce Rayner 2, Sourabh
More informationThe PSP compact MOSFET model An update
The PSP compact MOSFET model An update Gert-Jan Smit, Andries Scholten, D.B.M. Klaassen NXP Semiconductors Ronald van Langevelde Philips Research Europe Gennady Gildenblat, Weimin Wu, Xin Li, Amit Jha,
More informationSimple and accurate modeling of the 3D structural variations in FinFETs
Simple and accurate modeling of the 3D structural variations in FinFETs Donghu Kim Electrical Engineering Program Graduate school of UNIST 2013 Simple and accurate modeling of the 3D structural variations
More informationP. R. Nelson 1 ECE418 - VLSI. Midterm Exam. Solutions
P. R. Nelson 1 ECE418 - VLSI Midterm Exam Solutions 1. (8 points) Draw the cross-section view for A-A. The cross-section view is as shown below.. ( points) Can you tell which of the metal1 regions is the
More informationComparative studies of Ge and Si p-channel metal oxide semiconductor field-effect-transistors with HfSiON dielectric and TaN metal gate
Comparative studies of Ge and Si p-channel metal oxide semiconductor field-effect-transistors with HfSiON dielectric and TaN metal gate Hu Ai-Bin( 胡爱斌 ) and Xu Qiu-Xia( 徐秋霞 ) Institute of Microelectronics,
More informationCMOS Technology for Computer Architects
CMOS Technology for Computer Architects Recap Technology Trends Lecture 2: Transistor Inverter Iakovos Mavroidis Giorgos Passas Manolis Katevenis FORTH-ICS (University of Crete) 1 2 Recap Threshold Voltage
More informationThin Film Transistors (TFT)
Thin Film Transistors (TFT) a-si TFT - α-si:h (Hydrogenated amorphous Si) deposited with a PECVD system (low temp. process) replaces the single crystal Si substrate. - Inverted staggered structure with
More informationThe Future of CMOS. David Pulfrey. CHRONOLOGY of the FET. Lecture Lilienfeld s patent (BG FET) 1965 Commercialization (Fairchild)
The Future of CMOS David Pulfrey 1 CHRONOLOGY of the FET 1933 Lilienfeld s patent (BG FET) 1965 Commercialization (Fairchild) 1991 The most abundant object made by mankind (C.T. Sah) 2003 The 10 nm FET
More informationDevice Models (PN Diode, MOSFET )
Device Models (PN Diode, MOSFET ) Instructor: Steven P. Levitan steve@ece.pitt.edu TA: Gayatri Mehta, José Martínez Book: Digital Integrated Circuits: A Design Perspective; Jan Rabaey Lab Notes: Handed
More information296 IEEE TRANSACTIONS ON NUCLEAR SCIENCE, VOL. 65, NO. 1, JANUARY 2018
296 IEEE TRANSACTIONS ON NUCLEAR SCIENCE, VOL. 65, NO. 1, JANUARY 2018 Scaling Effects on Single-Event Transients in InGaAs FinFETs Huiqi Gong, Student Member, IEEE, KaiNi, Student Member, IEEE, EnXiaZhang,
More informationJournal of Electron Devices, Vol. 18, 2013, pp JED [ISSN: ]
DrainCurrent-Id in linearscale(a/um) Id in logscale Journal of Electron Devices, Vol. 18, 2013, pp. 1582-1586 JED [ISSN: 1682-3427 ] SUITABILITY OF HIGH-k GATE DIELECTRICS ON THE DEVICE PERFORMANCE AND
More informationA final review session will be offered on Thursday, May 10 from 10AM to 12noon in 521 Cory (the Hogan Room).
A final review session will be offered on Thursday, May 10 from 10AM to 12noon in 521 Cory (the Hogan Room). The Final Exam will take place from 12:30PM to 3:30PM on Saturday May 12 in 60 Evans.» All of
More informationThe Devices. Jan M. Rabaey
The Devices Jan M. Rabaey Goal of this chapter Present intuitive understanding of device operation Introduction of basic device equations Introduction of models for manual analysis Introduction of models
More informationESE 570: Digital Integrated Circuits and VLSI Fundamentals
ESE 570: Digital Integrated Circuits and VLSI Fundamentals Lec 5: January 25, 2018 MOS Operating Regions, pt. 1 Lecture Outline! 3 Regions of operation for MOSFET " Subthreshold " Linear " Saturation!
More informationProspects for Ge MOSFETs
Prospects for Ge MOSFETs Sematech Workshop December 4, 2005 Dimitri A. Antoniadis Microsystems Technology Laboratories MIT Sematech Workshop 2005 1 Channel Transport - I D I D =WQ i (x 0 )v xo v xo : carrier
More informationPhysics an performance of III-V nanowire heterojunction TFETs including phonon and impurity band tails:
Physics an performance of III-V nanowire heterojunction TFETs including phonon and impurity band tails: An atomistic mode space NEGF quantum transport study. A. Afzalian TSMC, Leuven, Belgium (Invited)
More informationExtending the Era of Moore s Law
14 nm chip X SEM from www.intel.com/content/dam/www/public/us/en/documents/pdf/foundry/mark bohr 2014 idf presentation.pdf Extending the Era of Moore s Law Tsu Jae King Liu Department of Electrical Engineering
More informationLecture 3: CMOS Transistor Theory
Lecture 3: CMOS Transistor Theory Outline Introduction MOS Capacitor nmos I-V Characteristics pmos I-V Characteristics Gate and Diffusion Capacitance 2 Introduction So far, we have treated transistors
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 informationMOS Transistor I-V Characteristics and Parasitics
ECEN454 Digital Integrated Circuit Design MOS Transistor I-V Characteristics and Parasitics ECEN 454 Facts about Transistors So far, we have treated transistors as ideal switches An ON transistor passes
More informationElectronics with 2D Crystals: Scaling extender, or harbinger of new functions?
Electronics with 2D Crystals: Scaling extender, or harbinger of new functions? 1 st Workshop on Data Abundant Systems Technology Stanford, April 2014 Debdeep Jena (djena@nd.edu) Electrical Engineering,
More informationThere s Plenty of Room at the Bottom and at the Top
14 nm chip X SEM from www.intel.com/content/dam/www/public/us/en/documents/pdf/foundry/mark bohr 2014 idf presentation.pdf There s Plenty of Room at the Bottom and at the Top Tsu Jae King Liu Department
More informationFLCC Seminar. Spacer Lithography for Reduced Variability in MOSFET Performance
1 Seminar Spacer Lithography for Reduced Variability in MOSFET Performance Prof. Tsu-Jae King Liu Electrical Engineering & Computer Sciences Dept. University of California at Berkeley Graduate Student:
More informationDecemb er 20, Final Exam
Fall 2002 6.720J/3.43J Integrated Microelectronic Devices Prof. J. A. del Alamo Decemb er 20, 2002 - Final Exam Name: General guidelines (please read carefully b efore starting): Make sure to write your
More informationLecture 9. Strained-Si Technology I: Device Physics
Strain Analysis in Daily Life Lecture 9 Strained-Si Technology I: Device Physics Background Planar MOSFETs FinFETs Reading: Y. Sun, S. Thompson, T. Nishida, Strain Effects in Semiconductors, Springer,
More informationMicroelectronics Part 1: Main CMOS circuits design rules
GBM8320 Dispositifs Médicaux telligents Microelectronics Part 1: Main CMOS circuits design rules Mohamad Sawan et al. Laboratoire de neurotechnologies Polystim! http://www.cours.polymtl.ca/gbm8320/! med-amine.miled@polymtl.ca!
More informationPlanar View of Structural Degradation in GaN HEMT: Voltage, Time and Temperature Dependence
Planar View of Structural Degradation in GaN HEMT: Voltage, Time and Temperature Dependence Jungwoo Joh 1, Prashanth Makaram 2 Carl V. Thompson 2 and Jesús A. del Alamo 1 1 Microsystems Technology Laboratories,
More informationModeling Random Variability of 16nm Bulk FinFETs
Modeling Random Variability of 16nm Bulk FinFETs Victor Moroz, Qiang Lu, and Munkang Choi September 9, 2010 1 Outline 2 Outline 3 16nm Bulk FinFETs for 16nm Node Simulation domain 24nm fin pitch 56nm gate
More informationCMOS Inverter (static view)
Review: Design Abstraction Levels SYSTEM CMOS Inverter (static view) + MODULE GATE [Adapted from Chapter 5. 5.3 CIRCUIT of G DEVICE Rabaey s Digital Integrated Circuits,, J. Rabaey et al.] S D Review:
More informationS=0.7 [0.5x per 2 nodes] ESE370: Circuit-Level Modeling, Design, and Optimization for Digital Systems. Today. Scaling ITRS Roadmap
ESE370: Circuit-Level Modeling, Design, and Optimization for Digital Systems Day 15: October 4, 2013 Scaling Today VLSI Scaling Trends/Disciplines Effects Alternatives (cheating) 1 2 Scaling ITRS Roadmap
More informationNanometer Transistors and Their Models. Jan M. Rabaey
Nanometer Transistors and Their Models Jan M. Rabaey Chapter Outline Nanometer transistor behavior and models Sub-threshold currents and leakage Variability Device and technology innovations Nanometer
More informationECE 497 JS Lecture - 12 Device Technologies
ECE 497 JS Lecture - 12 Device Technologies Spring 2004 Jose E. Schutt-Aine Electrical & Computer Engineering University of Illinois jose@emlab.uiuc.edu 1 NMOS Transistor 2 ρ Source channel charge density
More informationDevice Models (PN Diode, MOSFET )
Device Models (PN Diode, MOSFET ) Instructor: Steven P. Levitan steve@ece.pitt.edu TA: Gayatri Mehta, José Martínez Book: Digital Integrated Circuits: A Design Perspective; Jan Rabaey Lab Notes: Handed
More informationSimple Theory of the Ballistic Nanotransistor
Simple Theory of the Ballistic Nanotransistor Mark Lundstrom Purdue University Network for Computational Nanoechnology outline I) Traditional MOS theory II) A bottom-up approach III) The ballistic nanotransistor
More informationJFET/MESFET. JFET: small gate current (reverse leakage of the gate-to-channel junction) More gate leakage than MOSFET, less than bipolar.
JFET/MESFET JFET: small gate current (reverse leakage of the gate-to-channel junction) More gate leakage than MOSFET, less than bipolar. JFET has higher transconductance than the MOSFET. Used in low-noise,
More information! MOS Capacitances. " Extrinsic. " Intrinsic. ! Lumped Capacitance Model. ! First Order Capacitor Summary. ! Capacitance Implications
ESE 570: Digital Integrated Circuits and VLSI Fundamentals Lec 7: February, 07 MOS SPICE Models, MOS Parasitic Details Lecture Outline! MOS Capacitances " Extrinsic " Intrinsic! Lumped Capacitance Model!
More informationENGR890 Digital VLSI Design Fall Lecture 4: CMOS Inverter (static view)
ENGR89 Digital VLSI Design Fall 5 Lecture 4: CMOS Inverter (static view) [Adapted from Chapter 5 of Digital Integrated Circuits, 3, J. Rabaey et al.] [Also borrowed from Vijay Narayanan and Mary Jane Irwin]
More informationESE 570: Digital Integrated Circuits and VLSI Fundamentals
ESE 570: Digital Integrated Circuits and VLSI Fundamentals Lec 7: February 4, 2016 MOS SPICE Models, MOS Parasitic Details Lecture Outline! MOS Capacitances " Extrinsic " Intrinsic! Lumped Capacitance
More informationRecent Progress in Understanding the DC and RF Reliability of GaN High Electron Mobility Transistors
Recent Progress in Understanding the DC and RF Reliability of GaN High Electron Mobility Transistors J. A. del Alamo and J. Joh* Microsystems Technology Laboratories, MIT, Cambridge, MA *Presently with
More information6.012 Electronic Devices and Circuits
Page 1 of 10 YOUR NAME Department of Electrical Engineering and Computer Science Massachusetts Institute of Technology 6.012 Electronic Devices and Circuits Exam No. 2 Thursday, November 5, 2009 7:30 to
More informationLecture 4: CMOS Transistor Theory
Introduction to CMOS VLSI Design Lecture 4: CMOS Transistor Theory David Harris, Harvey Mudd College Kartik Mohanram and Steven Levitan University of Pittsburgh Outline q Introduction q MOS Capacitor q
More information