Nanoscale memory cell based on a nanoelectromechanical switched capacitor EECS Min Hee Cho.

Slides:



Advertisements
Similar presentations
MICROWAVE FET Microwave FET : operates in the microwave frequencies
Advertisements

by Alexander Glavtchev
6.1 Transistor Operation 6.2 The Junction FET
SOGANG UNIVERSITY SOGANG UNIVERSITY. SEMICONDUCTOR DEVICE LAB. Power MOSFET (3) SD Lab. SOGANG Univ. BYUNGSOO KIM.
Single Electron Devices Vishwanath Joshi Advanced Semiconductor Devices EE 698 A.
Metal Oxide Semiconductor Field Effect Transistors
Derek Wright Monday, March 7th, 2005
Carbon nanotube field effect transistors (CNT-FETs) have displayed exceptional electrical properties superior to the traditional MOSFET. Most of these.
Chun-Chieh Lu Carbon-based devices on flexible substrate 1.
High-K Dielectrics The Future of Silicon Transistors
GRAPHENE TRANSISTORS AND MEMORY. MOORE’S LAW THE PROBLEM 1. Reduction in saturation mode drain current. 2. Variation in Carrier velocity. 3. Modification.
Lateral Asymmetric Channel (LAC) Transistors
Cell and module construction. Photovoltaic effect and basic solar cell parameters To obtain a potential difference that may be used as a source of electrical.
Optimization of Carbon Nanotube Field-Effect Transistors (FETs) Alexandra Ford NSE 203/EE 235 Class Presentation March 5, 2007.
Spring 2007EE130 Lecture 35, Slide 1 Lecture #35 OUTLINE The MOS Capacitor: Final comments The MOSFET: Structure and operation Reading: Chapter 17.1.
Introduction to CMOS VLSI Design Lecture 0: Introduction
Interconnect Focus Center e¯e¯ e¯e¯ e¯e¯ e¯e¯ SEMICONDUCTOR SUPPLIERS Goal: Fabricate and perform electrical tests on various interconnected networks of.
Single Electron Transistor
Diodes Properties of SWNT Networks Bryan Hicks. Diodes and Transistors An ever increasing number in an ever decreasing area.
Week 8b OUTLINE Using pn-diodes to isolate transistors in an IC
Lecture 0: Introduction. CMOS VLSI Design 4th Ed. 0: Introduction2 Introduction  Integrated circuits: many transistors on one chip.  Very Large Scale.
Technologies for Realizing Carbon Nano-Tube (CNT) Vias Clarissa Cyrilla Prawoto 26 November 2014.
Introduction Integrated circuits: many transistors on one chip.
Optional Reading: Pierret 4; Hu 3
CMOS Process Integration ECE/ChE 4752: Microelectronics Processing Laboratory Gary S. May March 25, 2004.
Metal-Oxide-Semiconductor Field Effect Transistors
Z. Feng VLSI Design 1.1 VLSI Design MOSFET Zhuo Feng.
MOS Capacitors MOS capacitors are the basic building blocks of CMOS transistors MOS capacitors distill the basic physics of MOS transistors MOS capacitors.
Tutorial 8 Derek Wright Wednesday, March 9 th, 2005.
Philip Kim Department of Physics Columbia University Toward Carbon Based Electronics Beyond CMOS Devices.
VFET – A Transistor Structure for Amorphous semiconductors Michael Greenman, Ariel Ben-Sasson, Nir Tessler Sara and Moshe Zisapel Nano-Electronic Center,
Lecture 0: Introduction. CMOS VLSI Design 4th Ed. 0: Introduction2 Introduction  Integrated circuits: many transistors on one chip.  Very Large Scale.
Introduction to FinFet
IC Process Integration
Limitations of Digital Computation William Trapanese Richard Wong.
S. E. Thompson EEL 6935 Today’s Subject Continue on some basics on single-wall CNT---- chiral length, angle and band gap; Other properties of CNT; Device.
1 Recent studies on a single-walled carbon nanotube transistor Reference : (1) Mixing at 50GHz using a single-walled carbon nanotube transistor, S.Rosenblatt,
EE235 Presentation I CNT Force Sensor Ting-Ta YEN Feb Y. Takei, K. Matsumoto, I. Shimoyama “Force Sensor Using Carbon Nanotubes Directly Synthesized.
Lecture 24a, Slide 1EECS40, Fall 2004Prof. White Lecture #24a OUTLINE Device isolation methods Electrical contacts to Si Mask layout conventions Process.
Carbon nanotube is a magic material. The unique structure brings it amazing characteristics. Lots of people believe that the usage of carbon nanotube will.
Carbon Nanotubes Related Devices and Applications
Lecture 23 OUTLINE The MOSFET (cont’d) Drain-induced effects Source/drain structure CMOS technology Reading: Pierret 19.1,19.2; Hu 6.10, 7.3 Optional Reading:
Application of Silicon-Germanium in the Fabrication of Ultra-shallow Extension Junctions of Sub-100 nm PMOSFETs P. Ranade, H. Takeuchi, W.-H. Lee, V. Subramanian,
ADVANCED HIGH DENSITY INTERCONNECT MATERIALS AND TECHNIQUES DIVYA CHALLA.
Electro-Ceramics Lab. Electrical Properties of SrBi 2 Ta 2 O 9 Thin Films Prepared by r.f. magnetron sputtering Electro-ceramics laboratory Department.
March 3rd, 2008 EE235 Nanofabrication, University of California Berkeley Hybrid Approach of Top Down and Bottom Up to Achieve Nanofabrication of Carbon.
CMOS FABRICATION.
UTB SOI for LER/RDF EECS Min Hee Cho. Outline  Introduction  LER (Line Edge Roughness)  RDF (Random Dopant Fluctuation)  Variation  Solution – UTB.
The Fate of Silicon Technology: Silicon Transistors Maria Bucukovska Scott Crawford Everett Comfort.
Chieh Chang EE 235 – Presentation IMarch 20, 2007 Nanoimprint Lithography for Hybrid Plastic Electronics Michael C. McAlpine, Robin S. Friedman, and Charles.
Ali Javey, SungWoo Nam, Robin S.Friedman, Hao Yan, and Charles M. Lieber Ting-Ta Yen.
Fatemeh (Samira) Soltani University of Victoria June 11 th
UNIT II : BASIC ELECTRICAL PROPERTIES
Power MOSFET Pranjal Barman.
MOS Field-Effect Transistors (MOSFETs)
S-RCAT(Sphere-shaped-Recess-Channel-Array-Transistor) Technology for 70nm DRAM feature size and beyond J.Y.Kim and Kinam Kim, et all (Samsung Electronics)
Prof. Haung, Jung-Tang NTUTL
Metal Semiconductor Field Effect Transistors
by Alexander Glavtchev
M. Mahmoodi1, M. Arjmand2, U. Sundararaj2 and S. S. Park1
INTRODUCTION: MD. SHAFIQUL ISLAM ROLL: REGI:
Nanowire Gate-All-Around (GAA) FETs
Optional Reading: Pierret 4; Hu 3
Lecture #25 OUTLINE Device isolation methods Electrical contacts to Si
Lecture 19 OUTLINE The MOS Capacitor (cont’d) The MOSFET:
(2) Incorporation of IC Technology Example 18: Integration of Air-Gap-Capacitor Pressure Sensor and Digital readout (I) Structure It consists of a top.
SILICON MICROMACHINING
Lecture 19 OUTLINE The MOS Capacitor (cont’d) The MOSFET:
Beyond Si MOSFETs Part IV.
Beyond Si MOSFETs Part 1.
Presentation transcript:

Nanoscale memory cell based on a nanoelectromechanical switched capacitor EECS Min Hee Cho

Outline I Introduction Agenda DRAM & Key idea Capacitor type Carbon Nanotube II Mechanical switched capacitor Fabrication SEM image Operation Switching characteristics J. E. Jang, et al. nature nanotechnology 2008 (Samsung Advanced Institute of Technology & U of Cambridge ) J. E. Jang, et al. APPLIED PHYSICS LETTERS 2008 III Low voltage drive Low Gate Voltage Fabrication SEM image IV Summary Summary : Merits Summary : remaining obstacles V References/ Q&A

Outline I Introduction Agenda DRAM & Key idea Capacitor structure Carbon Nanotube II Mechanical switched capacitor Fabrication SEM image Operation Switching characteristics III Low voltage drive Low Gate Voltage Fabrication SEM image IV Summary Summary : Merits Summary : remaining obstacles V References/ Q&A

Agenda Conventional DRAMNew DRAM FabricationTop-Down processBottom-Up Process (CNT) OperationField Effect Transistor + Capacitor Electromechanical switch + Capacitor Nanoscale memory cell = DRAM with Carbon nanotube

DRAM & Key idea Schematic drawing of original designs of DRAM patented in * Development of DRAM : Cell size is smaller and smaller  TR : On/Off ratio ↓(due to Short channel effect)  Cap : Area of capacitor is also reduced ( Capacitor should be larger to improve performance) * Solution  TR : Mechanical switched TR  Cap: Vertical structure ( increase area of capacitor ) or High K Gate Drain Source Capacitor

Trench type Capacitor structure Cylinder type like “HAT” Dielectric :small area

Gate Drain Source Capacitor SourceDrain Gate DRAM has several limits as shrinkage * Transistor - low Subthreshold swing (low On/Off ratio) - short channel effect (Off leakage) New challenge for DRAM with CNT * Transistor - Use Electromechanical property not Field effect  On/Off ratio ↑ - Smaller cell area : due to the vertical structure * Additionally, they can use existing silicon technology Area also reduced Conventional DRAM structure New DRAM structure New DRAM structure

Carbon Nanotube (CNT) Properties Single WalledCarbon Nanotube (SWNT) Multi-Walled Carbon Nanotube (MWNT) Comparison Diameter (nm)1.2~35~100 Hair (70~100)×10 3 Tension (GPa)~45<50~300 Stainless steel : 0.65~1) Density(g/cc)1.33~1.40-Al ~2.7 Electric resistance (Ω·m) 10× ×10 -8 Cu 1.7×10 -8 Current density (A/m 2 ) ~109-Cu 106 Thermal conductivity( W/m·K) ~6000~3000 Diamond : 2000~40000, Cu: They use CNT as electromechanical materials rather than semiconductor material

Outline I Introduction Agenda DRAM & Key idea Capacitor type Carbon Nanotube II Mechanical switched capacitor Fabrication SEM image Operation Switching characteristics III Low voltage drive Low Gate Voltage Fabrication SEM image IV Summary Summary : Merits Summary : remaining obstacles V References/ Q&A

Fabrication 0. Make Nb catalyst dot on Substrate I. C 2 H 2 &NH 3 gas 600~650 o C by PECVD : CNT II. Si 3 N 4 (dielectric & insulator) by PECVD III. Cr by sputtering : upper electrode IV. Si 3 N 4 at Drain removed by wet etching  Si 3 N 4 remaining at bottom of MWCNT strengthen the interface  enhance working reliability

SEM image

* Total cell: 40,000 ea * MWCNT success rate : 95% * Final cell success rate : 50% (failure due to mainly M/A in litho) CNT diameter : 70nm Gap between CNT : 100nm Length : 3.5um Si 3 N 4 thickness : 40nm For single capacitance: 1.05fF SEM images

Outline I Introduction Agenda DRAM & Key idea Capacitor type Carbon Nanotube II Mechanical switched capacitor Fabrication SEM image Operation Switching characteristics III Low voltage drive Low Gate Voltage Fabrication SEM image IV Summary Summary : Merits Summary : remaining obstacles V References/ Q&A

Write Operation The mutual repulsion between the positive charges on the capacitor and the nanotube in cell 1 prevents the nanotube from making contact with the capacitor, so no current flows, unlike the situation in cell 2, where the nanotube does make contact with the cell. Read Write BL of Cell 1 and  apply 0.1V  gate voltage to the 15V  CNT of Cell 1 begins to bend  contacts  charges flow from CNT(BL) to capacitor

* When gate voltage is higher than Vt, Transistor turns on * Vd increase  Vt decreases due to electrostatic force Threshold gate voltage (Vt) OFF ONON Very High gate voltage : Usually DRAM operates at ~1.3V (or less than 2.5V) Switching characteristics

Outline I Introduction Agenda DRAM & Key idea Capacitor type Carbon Nanotube II Mechanical switched capacitor Fabrication SEM image Operation Switching characteristics III Low voltage drive Low Gate Voltage Fabrication SEM image IV Summary Summary : Merits Summary : remaining obstacles V References/ Q&A J. E. Jang, et al. APPLIED PHYSICS LETTERS 2008

Low Gate Voltage Too high operating voltage (15~20V) APPLIED PHYSICS LETTERS 93, ∵ The simple planar gate structure imparts a very small electrostatic force to the drain  electrostatic force ∝ 1/d 2  Need high voltage Vertical gate structure In this work They make vertical gate and tie it with drain

14~15V 4~5 V

PolyMethyl MethAcrylate (PMMA) : thermoplastic and transparent plastic. PMMA coating after the CNT growth pr ocess. 30 nm SiNx deposition by PECV D E-beam lithography with substrate tilting Cr layer deposition lift-off process (Cr on PMMA removed) 400 nm PMMA coating and ashing process to remove the Thin PMMA on the vertical CNT and gate structure Fabrication

1> Operating Gate voltage can be reduced2> Area also reduced SEM images

Outline I Introduction Agenda DRAM Memory Basic Operation Capacitor type Carbon Nanotube II Mechanical switched capacitor Fabrication SEM image Operation Switching characteristics III Low voltage drive Low Gate Voltage Fabrication SEM image IV Summary Summary : Merits Summary : remaining obstacles V References/ Q&A

Summary : Merits Excellent ‘ON–OFF’ ratio – Due to the mechanical switching approach  No ultra-shallow n- or p-type junctions  No thin-gate dielectrics Compatible with existing silicon technology Vertical orientation  Cell area ↓ Placing defined numbers of nanotubes at selected locations

Summary : Remaining Obstacles High voltage  Vertical gate (14V  4V : still high) The growth temperature used in this work : 600–650 o C is relatively high for integration with CMOS technology Still larger (~200nm ) : Need demonstration at smaller size is needed Randomization of nanotube orientation by thermal fluctuations and gas flows

References “ Nanoscale memory cell based on a nanoelectromechanical switched capacitor”, J. E. Jang, et al. (Samsung Advanced Institute of Technology & U of Cambridge) Nature 26 Nanotechnology | VOL 3 | JANUARY 2008 “Nanoelectromechanical switch with low voltage drive” J. E. Jang, et al. APPLIED PHYSICS LETTERS 93, Internet search – DRAM / CNT etc.

Thank you very much See you again! Q&A