Optical Proximity Correction

Similar documents
Introduction. Photoresist : Type: Structure:

UNIVERSITY OF CALIFORNIA College of Engineering Department of Electrical Engineering and Computer Sciences. Professor Ali Javey. Spring 2009.

Lecture 8. Photoresists and Non-optical Lithography

Techniken der Oberflächenphysik (Techniques of Surface Physics)

Photolithography 光刻 Part II: Photoresists

UNIT 3. By: Ajay Kumar Gautam Asst. Prof. Dev Bhoomi Institute of Technology & Engineering, Dehradun

5. Photochemistry of polymers

Introduction to Photolithography

MSN551 LITHOGRAPHY II

Pattern Transfer- photolithography

Lecture 14 Advanced Photolithography

MICRO AND NANOPROCESSING TECHNOLOGIES

MEEN Nanoscale Issues in Manufacturing. Lithography Lecture 1: The Lithographic Process

IC Fabrication Technology

Table of Contents. Foreword... Jörge DE SOUSA NORONHA. Introduction... Michel BRILLOUËT

Top down and bottom up fabrication

Lithography and Etching

The Monte Carlo Simulation of Secondary Electrons Excitation in the Resist PMMA

Photomasks. Photolithography Evolution 9/11/2004 ECE580- MPE/MASKS/PHOTOMASKS.PPT

Reactive Ion Etching (RIE)

There's Plenty of Room at the Bottom

Photolithography Overview 9/29/03 Brainerd/photoclass/ECE580/Overvie w/overview

Nanostructures Fabrication Methods

Chapter 3 : ULSI Manufacturing Technology - (c) Photolithography

Development of Lift-off Photoresists with Unique Bottom Profile

UNIVERSITY OF CALIFORNIA College of Engineering Department of Electrical Engineering and Computer Sciences. Fall Exam 1

Nano fabrication by e-beam lithographie

UNIVERSITY OF CALIFORNIA College of Engineering Department of Electrical Engineering and Computer Sciences. Professor Ali Javey. Fall 2009.

Nanoimprint Lithography

Supplementary Information Our InGaN/GaN multiple quantum wells (MQWs) based one-dimensional (1D) grating structures

EE115C Winter 2017 Digital Electronic Circuits. Lecture 3: MOS RC Model, CMOS Manufacturing

EE141- Spring 2003 Lecture 3. Last Lecture

520/ Photolithography (II) Andreas G. Andreou

Lecture 150 Basic IC Processes (10/10/01) Page ECE Analog Integrated Circuits and Systems P.E. Allen

Photolithography II ( Part 1 )

Make sure the exam paper has 9 pages (including cover page) + 3 pages of data for reference

EE143 LAB. Professor N Cheung, U.C. Berkeley

Introduction to Electron Beam Lithography

Carrier Transport by Diffusion

DQN Positive Photoresist

CURRENT STATUS OF NANOIMPRINT LITHOGRAPHY DEVELOPMENT IN CNMM

Techniques for directly measuring the absorbance of photoresists at EUV wavelengths

Overview of the main nano-lithography techniques

Section 3: Etching. Jaeger Chapter 2 Reader

FLCC Seminar. Spacer Lithography for Reduced Variability in MOSFET Performance

4FNJDPOEVDUPS 'BCSJDBUJPO &UDI

EE130: Integrated Circuit Devices

EE C245 ME C218 Introduction to MEMS Design Fall 2007

High NA the Extension Path of EUV Lithography. Dr. Tilmann Heil, Carl Zeiss SMT GmbH

Fabrication Engineering at the Micro- and Nanoscale, by Stephen Campbell, 4 th Edition, Oxford University Press

Far IR Gas Lasers microns wavelengths, THz frequency Called Terahertz lasers or FIR lasers At this wavelength behaves more like

Make sure the exam paper has 7 pages (including cover page) + 3 pages of data for reference

EE 434 Lecture 7. Process Technology

Fabrication-II. Electron Beam Lithography Pattern Design Thin Film Deposition

Wet Chemical Processing with Megasonics Assist for the Removal of Bumping Process Photomasks

After Development Inspection (ADI) Studies of Photo Resist Defectivity of an Advanced Memory Device

Ion Implantation. alternative to diffusion for the introduction of dopants essentially a physical process, rather than chemical advantages:

ORION NanoFab: An Overview of Applications. White Paper

Technologies VII. Alternative Lithographic PROCEEDINGS OF SPIE. Douglas J. Resnick Christopher Bencher. Sponsored by. Cosponsored by.

Chromeless Phase Lithography (CPL)

Etching: Basic Terminology

EE C247B / ME C218 INTRODUCTION TO MEMS DESIGN SPRING 2016 C. NGUYEN PROBLEM SET #4

Fabrication Technology, Part I

Sensors and Metrology. Outline

Development of Photosensitive Polyimides for LCD with High Aperture Ratio. May 24, 2004

Developer-soluble Gap fill materials for patterning metal trenches in Via-first Dual Damascene process

Design of Attenuated Phase-shift shift Mask with ITO Absorber for Extreme Ultraviolet Lithography

Resist material for negative tone development process

Photoresist Profile. Undercut: negative slope, common for negative resist; oxygen diffusion prohibits cross-linking; good for lift-off.

Process-Simulation-Flow And Metrology of VLSI Layout Fine- Features

A Novel Approach to the Layer Number-Controlled and Grain Size- Controlled Growth of High Quality Graphene for Nanoelectronics

Current Status of Inorganic Nanoparticle Photoresists

Technology for Micro- and Nanostructures Micro- and Nanotechnology

J. Photopolym. Sci. Technol., Vol. 22, No. 5, Fig. 1. Orthogonal solvents to conventional process media.

Silicon VLSI Technology. Fundamentals, Practice and Modeling

Enhanced Transmission by Periodic Hole. Arrays in Metal Films

Chapter 2 Process Variability. Overview. 2.1 Sources and Types of Variations

Composition and Photochemical Mechanisms of Photoresists

Far IR (FIR) Gas Lasers microns wavelengths, THz frequency Called Terahertz lasers or FIR lasers At this wavelength behaves more like

Direct write electron beam patterning of DNA complex thin films

Fabrication of ordered array at a nanoscopic level: context

Recent progress in nanoparticle photoresist development for EUV lithography

Study of Iso/Dense Bias of BARCs and Gap-Fill Materials on Via Wafers Runhui Huang, Brewer Science, Inc Brewer Dr., Rolla, MO 65401, USA

Self-study problems and questions Processing and Device Technology, FFF110/FYSD13

Chen et al. (45) Date of Patent: Dec. 5, (54) EFFECTIVE PHOTORESIST STRIPPING (56) References Cited

Micro- and Nano-Technology... for Optics

Swing Curves. T h e L i t h o g r a p h y T u t o r (Summer 1994) Chris A. Mack, FINLE Technologies, Austin, Texas

Wet and Dry Etching. Theory

Dry Etching Zheng Yang ERF 3017, MW 5:15-6:00 pm

Large Scale Direct Synthesis of Graphene on Sapphire and Transfer-free Device Fabrication

EUREKA: A new Industry EUV Research Center at LBNL

Lab1. Resolution and Throughput of Ion Beam Lithography.

Photonics applications 5: photoresists

EE C245 ME C218 Introduction to MEMS Design Fall 2007

Three Approaches for Nanopatterning

Nano Materials. Nanomaterials

EE 143 MICROFABRICATION TECHNOLOGY FALL 2014 C. Nguyen PROBLEM SET #7. Due: Friday, Oct. 24, 2014, 8:00 a.m. in the EE 143 homework box near 140 Cory

Chapter 3 Basics Semiconductor Devices and Processing

High Yield Structured X-ray Photo-Cathode Development and Fabrication

Lecture 0: Introduction

Transcription:

Optical Proximity Correction Mask Wafer *Auxiliary features added on mask 1

Overlay Errors + + alignment mask wafer + + photomask plate Alignment marks from previous masking level 2

(1) Thermal run-in/run-out errors R r Tm m Tsi si run-out wafer error radius Tm, Tsi change of mask and wafer temp. m, si coefficient of thermal expansion of mask & Si 3

run-out (2) Translational Error Al n+ p image referrer 4

(3) Rotational Error 5

6

Characterization of Overlay Errors T O + y x R L O + + O C + O O + R O =optical image + =alignment marks on wafer wafer B 7

Example m x y T 0.0 0.7 R 0.7 1.0 C 0.5 0.5 L 0.3 0.0 B 1.0 0.3 * Center of wafer has only translation error Terror = (0.5, 0.5) After subtracting Terror, 8

T -0.5 0.2 x y T R 0.2 0.5 C 0 0 B 0.5-0.2 y x 0.5 R L L -0.2-0.5 0.2 B wafer 9

Run out error 0.2 m Rotational error 0.5 m [counter clockwise] If wafer diameter is 4" D 10 cm Rotational error 5 10 radians y R 10

Optical image of mask alignment marks Reference marks on wafer With thermal run-out, the alignment error is 1/2 of the image/reference difference [best scenario] 11

Total Overlay Tolerance 2 i total 2 i th masking step = std. deviation of overlay error for i i total = std. deviation for total overlay error Layout design-rule specification should be > total 12

Example: Contact to source/drain of MOSFET. SiO2 SiO2 Al ideal n+ p-si SiO2 Alignment error between oxide opening and n+ pattern SiO2 n+ Al short, ohmic contact p-si 13

Solution: Design n+ region larger than contact hole Al SiO2 SiO2 n+ 14

Two Resist Types Negative Resist Polymer (Molecular Weight (MW) ~65000) Light Sensitive Additive Promotes Crosslinking Volatile Solvents Light breaks N-N => Crosslink Chains Sensitive, hard, Swelling during Develop Positive Resist Polymer (MW~5000) Photoactive Inhibitor (20%) Volatile Solvents Inhibitor Looses N2 => Alkali Soluble Acid Develops by etching - No Swelling. 15

Positive Resist hv mask exposed part is removed 100% (linear scale) E1 P.R. ET = resist sensitivity Resist contrast LOG TO BASE 10 log resist thickness remaining ET exposure photon energy (log scale) ~ 5 to 10 Note: In the 143 Reader, is defined as natural log 16

Positive P.R. Mechanism Photons deactivate sensitizer less cross-linking dissolve in developer solution polymer + photosensitizer 17

diazide Positive Resist Exposure Reaction ketene - a = C = 0 group The ketene is shortlived intermediate PAC carboxylic acid moisture The carboxylic acid can react with the alkaline solution (the soluble ester developer) to form a soluble ester. 18

Chemical Amplified Resist (CAR) For reference only Photo-Acid generator 19 N Cheung EE243 s2010 L

Negative P.R. Mechanism hv % remaining mask after development ET 1 E1 log ET E1 photon energy hv => cross-linking => insoluble in developer solution. Log to base 10 20

Why High-Contrast Resist is desirable? Optical image Infinite contrast resist resist substrate Finite contrast resist resist substrate Position x 21

22

Positive vs. Negative Photoresists Positive P.R.: higher resolution aqueous-based solvents less sensitive Negative P.R.: more sensitive => higher exposure throughput relatively tolerant of developing conditions better chemical resistance => better mask material less expensive lower resolution organic-based solvents 23

Standing Waves *Photoresist has a finite thickness hv Higher Intensity Faster Development rate Lower Intensity Slower Development rate Positive Photoresist substrate Positive Photoresist. After development substrate 24

Standing reflecting wave effect surface Air Photoresist E E E Resist profile and energy deposition depend on oxide thickness underneath (see handout for derivation) 4 3 E 1 Oxide 2 x=0 x=d r x=d T 1 I23 (x) = (E (x)+e3(x))2dt T 2 I23 (max) 0 1 = (E2 - E3)2 + 2E2E3sin2[k(d-x)] 2 1 1 I23 (max) = (E2 + E3)2 ; I 23(min) = (E2 - E3)2 2 2 I23 (min) x 2 n In ten sity m in im a occu r at : (d -x) = 0,, 2,... 2 n In ten sity m a x im a occu r a t : (d -x ) = /2, 3, 5,... d 25

x P.R. d SiO2/Si substrate Intensity = minimum when x d m Intensity = maximum when x d m n = refractive index of resist 2n 4n m = 0, 1, 2,... m = 1, 3, 5,... 26

Simulated Resist Cross-section as function of development time 27

Proximity Scattering 28

Approaches for Reducing Substrate Effects Use absorption dyes in photoresist Use anti-reflection coating (ARC) Use multi-layer resist process 1: thin planar layer for high-resolution imaging (imaging layer) 2: thin develop-stop layer, used for pattern transfer to 3 (etch stop) 3: thick layer of hardened resist (planarization layer) 29

Electron-Beam Lithography 12.3 V Angstroms for V in Volts Example: 30 kv e-beam => = 0.07 Angstroms NA = 0.002 0.005 Resolution < 1 nm But beam current needs to be 10 s of ma for a throughput of more than 10 wafers an hour. 30

Low Throughput for both raster and vector scanning (Serial Process) Variable Beam-shape EBL Stencil Mask EBL 31

The Proximity Effect Monte Carlo simulation of electron trajectories 32

e-beam lithography resolution factors beam quality ( ~1 nm) secondary electrons ( lateral range: few nm) performance records organic resist PMMA ~ inorganic resist, b.v. AlF3 ~ 7 nm 1-2 nm 33

Immersion Lithography A liquid with index of refraction n>1 is introduced between the imaging optics and the wafer. liquid = air /n With water, the index of refraction at = 193 nm is 1.44, improving the resolution significantly. 34

Phase-Shifting Mask For resolution enhancement. Example shown is an alternating PSM

EUV Lithography =11.2 nm 36

Schematic for EUV Litho Mo-Si Reflective Mask reflectivity 37 N Cheung EE243S05 Lec

Nanoimprinting 38 N Cheung EE243S05 Lec

Why photolithography? High throughput Empirical : Resolution (in Å) ~ 23 Areal Throughput (in um2/hr) 0.2 39 N Cheung EE243S05 Lec

40

Hands On Exploration of Images http://cuervo.eecs.berkeley.edu/ A web browser-based simulator of lithography 41