Experimental Characterization of Topography Induced Immersion Bubble Defects

Similar documents
NNCI ETCH WORKSHOP SI DRIE IN PLASMATHERM DEEP SILICON ETCHER. Usha Raghuram Stanford Nanofabrication Facility Stanford, CA May 25, 2016

Water for Immersion Lithography

EUV Resist Performance under High Stray Light Levels: an Interference Lithography Study

EUV Mask Handling Standards

High Aspect Ratio DRIE on the STS ICP-RIE

Quartz etch process to improve etch depth linearity and uniformity using Mask Etcher IV

1999 Microcomponents Technology SLYA017A

Outline Chapter 7 Waves

Understanding How the Appearance of Optical Fiber Splices Relates to Splice Quality

Figure 2: Principle of GPVS and ILIDS.

Bill Williams FMTC Probe Technology Development Group

CENTER PIVOT EVALUATION AND DESIGN

Application of CFD for Improved Vertical Column Induced Gas Flotation (IGF) System Development

Computer Simulation Helps Improve Vertical Column Induced Gas Flotation (IGF) System

FT28_mks.qxp 21/11/ :06 Page 1

Wind Loading of Large Telescopes

OPTIMIZATION OF RECUPERATER FIN GEOMETRY FOR MICRO GAS TURBINE

Second International Symposium Antwerp, 30 September-2 October Opening. Robert A. Hartman

(OBPL: Out of Band Protection Layer) Ryuji Onishi, Rikimaru Sakamoto, Noriaki Fujitani, Takafumi Endo, Bang-ching Ho

Air Bubble Defects in Dispensing Nanoimprint Lithography

SIMULATION OF ENTRAPMENTS IN LCM PROCESSES

Study of air bubble induced light scattering effect on the image quality in 193 nm immersion lithography

SMART Pad for CMP. Sunghoon Lee 1, David A. Dornfeld 1 Hae Do Jeong 2. University of California, Berkeley, USA 2

The Evolution of Vertical Spatial Coherence with Range from Source

2.830J / 6.780J / ESD.63J Control of Manufacturing Processes (SMA 6303) Spring 2008

Glass Frit Wafer Bonding Sealed Cavity Pressure in Relation to Bonding Process Parameters. Roy Knechtel, Sophia Dempwolf, Holger Klingner

Deep Trench Metrology Challenges for 75nm DRAM Technology Peter Weidner, Alexander Kasic, Thomas Hingst Thomas Lindner, Qimonda, Dresden, Germany

EXPERIMENTAL RESULTS OF GUIDED WAVE TRAVEL TIME TOMOGRAPHY

Yoke Instrumentation: ILD Muon System / Tail Catcher. Valeri Saveliev IAM, RAS, Russia DESY, Germany 3 June, 2016

Resist Outgassing and its Role in Optics Contamination

REACTIVE ION ETCHING OF SILICON DIOXIDE USING BOTH OXYGEN AND CARBON DIOXIDE AS GAS ADDITIVES. dames E. Constantino ABSTRACT

Aalborg Universitet. Published in: Proceedings of Offshore Wind 2007 Conference & Exhibition. Publication date: 2007

Numerical and Experimental Investigation of the Possibility of Forming the Wake Flow of Large Ships by Using the Vortex Generators

Impact of Lead Free on Automated X-Ray Inspection

Chapter 5: Methods and Philosophy of Statistical Process Control

Bonding Reliability Testing for Wafer Level Packaged MEMS Devices

Design and Technology Solutions for Development of SiGeMEMS devices. Tom Flynn Vice President, Sales Coventor

STS Advanced Oxide Etch DRIE System Trends

(Supplementary) Investigation Waves in a Ripple Tank

Off-gassing from III-V Wafer Processing -- A Collaboration of SEMATECH and IMEC

LOW PRESSURE EFFUSION OF GASES adapted by Luke Hanley and Mike Trenary

Assessment of correlations between NDE parameters and tube structural integrity for PWSCC at U-bends

STS ICP-RIE. Scott Munro (2-4826,

Impact of Reprocessing Technique on First Level Interconnects of Pb- Free to SnPb Reballed Area Array Flip Chip Devices

Hydraulic Modeling to Aid TDG Abatement at Boundary and Cabinet Gorge Dams

Investigating the Bubble Behavior in Pool Boiling in Microgravity Conditions Thilanka Munasinghe, Member, IAENG

Student Exploration: Ripple Tank

nearfield High-Throughput Atomic Force Microscopy for semiconductor metrology applications I N S T R U M E N T S

Air entrainment in Dip coating under vacuum

Micro-Venturi injector: design, experimental and simulative examination

Tools for safety management Effectiveness of risk mitigation measures. Bernhard KOHL

New University Based SRF Materials Research Efforts (in the US)

EMN04, October 2004, Paris, France OPTIMIZED ULTRA-DRIE FOR THE MEMS ROTARY ENGINE POWER SYSTEM

Using Spatio-Temporal Data To Create A Shot Probability Model

Photolithography. Operating Instructions

OPTIMIZATION OF INERT GAS FLOW INSIDE LASER POWDER BED FUSION CHAMBER WITH COMPUTATIONAL FLUID DYNAMICS. Abstract. Introduction

Best Practice for Calibrating LTH Conductivity Instruments

Simulation of Free Surface Flows with Surface Tension with ANSYS CFX

Modeling Approaches to Increase the Efficiency of Clear-Point- Based Solubility Characterization

Product Standard and Inspection Criteria for ilmasil PS Clear Fused Quartz Tubes

Figure 1 Schematic of opposing air bearing concept

Operation of the mask aligner MJB-55

SPECIFICATIONS PARTICLE SENSOR KS-18F Higashimotomachi, Kokubunji, Tokyo , Japan

Characterization and Modeling of Wafer and Die Level Uniformity in Deep Reactive Ion Etching (DRIE)

Ripple Tank Exploring the Properties of Waves Using a Ripple Tank

Workshop 1: Bubbly Flow in a Rectangular Bubble Column. Multiphase Flow Modeling In ANSYS CFX Release ANSYS, Inc. WS1-1 Release 14.

Separating Load from Moisture Effects in Wet Hamburg Wheel-Track Test

Unit 4: Inference for numerical variables Lecture 3: ANOVA

Analysis of Variance. Copyright 2014 Pearson Education, Inc.

Cell counts using Improved Neubauer haemocytometer

THEORETICAL EVALUATION OF FLOW THROUGH CENTRIFUGAL COMPRESSOR STAGE

Dynamic Modelling of Control Valves

Automating Injection Molding Simulation using Autonomous Optimization

Investigation of Cr Etch Chamber Seasoning Pavel Nesladek a, Guenther Ruhl b, Marcel Kristlib b

Resist round robin ELETTRA

Modelling of Extreme Waves Related to Stability Research

Introduction to topological data analysis

A decade of EUV resist outgas tes2ng Lessons learned. C. Tarrio, S. B. Hill, R. F. Berg, T. B. Lucatorto NIST, Gaithersburg, MD, USA

LOW PRESSURE EFFUSION OF GASES revised by Igor Bolotin 03/05/12

FEMA Region V. Great Lakes Coastal Flood Study. Pilot Study Webinar. Berrien County, Michigan. February 26, 2014

Background Statement for SEMI Document 5424A LINE ITEMS REVISION TO SEMI M , SPECIFICATIONS FOR SILICON EPITAXIAL WAFERS

Info Counting chamber (haemacytometer)

Overview. Learning Goals. Prior Knowledge. UWHS Climate Science. Grade Level Time Required Part I 30 minutes Part II 2+ hours Part III

MoLE Gas Laws Activities

Magical bubbles and soap films

Nature Neuroscience: doi: /nn Supplementary Figure 1. Visual responses of the recorded LPTCs

Are Detonator Qualification and Lot Acceptance Test Requirements Rational?

Technical Note. Determining the surface tension of liquids by measurements on pendant drops

J. J. Daly Metal Improvement Company Paramus New Jersey USA

Hydrogen Bubble Dispersion and Surface Bursting Behaviour

STRIDE PROJECT Steel Risers in Deepwater Environments Achievements

Flow transients in multiphase pipelines

Ermenek Dam and HEPP: Spillway Test & 3D Numeric-Hydraulic Analysis of Jet Collision

SOLAR 93 THE 1993 AMERICAN SOLAR ENERGY SOCIETY ANNUAL CONFERENCE. Washington, DC April 22028,1993. Editors: S. M. Burley M. E.

In ocean evaluation of low frequency active sonar systems

BILLY BISHOP TORONTO CITY AIRPORT PRELIMINARY RUNWAY DESIGN COASTAL ENGINEERING STUDY

Moving Towards Profitability

Modeling of thin strip profile during cold rolling on roll crossing and shifting mill

Pathogen Transport in Coastal Environments: Case Studies of Urban Runoff in Southern California

Double Emulsion Droplet generation and collection protocol Version Author Date Reviewer Change 1 Introduction

Transcription:

Experimental Characterization of Topography Induced Immersion Bubble Defects Michael Kocsis a, Christian Wagner b, Sjoerd Donders b, Tony DiBiase c, Alex Wei d, Mohamed El-Morsi d, Greg Nellis d, Roxann Engelstad d, Peter De Bisschop e a: Intel Corp, b: ASML, c: KLA Tencor, d: University of Wisconsin, e: IMEC 1

Why Are We Concerned? Bubbles New immersion specific defect mechanism. Effect of Topography: May increase the probability of bubble formation Bubbles on surface are stationary May have a longer lifetime than those suspended in liquid Simulation Presented at Jan 2004 Workshop 2

Surface Bubbles on Flat Wafers Immersion tests have been done on flat wafers. Bubble defects were detected with a bright field inspection tool. Non-Topography related Act as micro-lenses Test using a KLA PCM Reticle, inspected on a KT2360 3

Bubble Magnification Effect: Principles total internal reflection diffracts the rays at the outer rim Bubble Dia >> λ refraction leads to defocusing of the image: magnified projected image is printed 4

Bubble Magnification Effect: Data Pattern magnified, and unsharp Light missing, due to reflection No Bubble Defect With Bubble Defect See ASML Paper: Bubble Investigation for Immersion Lithography Sjoerd Donders, Richard Moerman 5

Surface Conditions Play an Important Role Both simulations and experimental data: probability of bubble formation increases with contact angle. Bubble Defects vs Contact Angle on Flat Wafers Number of Bubble Defects 10X Increase Hydrophillic (67 Degrees) Contact Angle Hydrophobic (117 Degrees) 6

Topography Wafers Create wafers with extreme topography to get a first look at how serious a problem entrained bubbles may be. Etched Oxide Trenches (150nm, 250nm), MT1 Test Reticle, 0.13um Design Rules, Line/Space Arrays, Very Limited Random Logic Structures Top Coat (41nm) 117 0 Contact Angle Resist (175nm) BARC (37nm) Oxide (150nm, 250nm) 0.125um-10.0um Silicon Worse case trench depth and contact angle. 7

Expose on 193nm Immersion Tool Immersion Prototype AT1150i Liquid containment Integrated Liquid Supply (temp, degassing, purity) Existing Lens modified for immersion Proven dry 3-D mapping of wafer surface 8

Experiment Run Plan Wafer Scanner Exposure 250nm Trench 193nm Immersion MT2 DF Reticle 150nm Trench 193nm Immersion MT2 DF Reticle 250nm Trench 193nm Immersion 1.5*E0 Open Frame 150nm Trench 193nm Immersion 1.5*E0 Open Frame Flat Test Wafer 193nm Immersion 1.5*E0 Open Frame 150nm Trench 193nm Dry 1.5*E0 Open Frame Open Frame: exposure of entire field area vs MT2 Dark Field reticle: ~30% exposure area. Flat wafers, and Dry exposures were used as comparisons to separate out non-topography related defects. 9

Topography Results Wafers were measured on a KT2360 Topography wafers exposed with open frame at 1.5xE0: high levels of residual resist remaining around the edges of the trenches; impossible to use for defect analysis. Topography wafers exposed with the MT2 reticle: high non-immersion related particle defect count non-optimum resist process, many defects could be filtered out of the data inspection sensitivity had to be detuned to prevent overload. 10

Topography Results The large bubble defects seen on the flat wafers were also seen on the topography wafer. Ref: No Defect Bubble Defect Late Breaking News: Some initial indication that these bubbles appear more frequently on certain areas within the field. 11

Topography Results The results have shown no evidence that any of the other defects found are caused by bubbles. Examples of typical defects, ~ 2000/wafer Smallest defects detected ~ 400nm (recipe had to be de-tuned to limit defect overload) 12

Does it match simulation results? Measured: Resist surface topography on the 250nm deep trench wafer with an (AFM). Dynamic contact angle of the top coat. Simulations: These conditions were then used by the UW Computational Mechanics Center to verify the results with CFD models that have been developed to predict when air will be entrained due to flow over topology. 13

400nm Line/250nm Space Array AFM Plot of Surface Topography 48nm Peak- Valley Simulation Results NO BUBBLES 14

3.0um Line/7.0um Space Array AFM Plot of Surface Topography 132nm Peak- Valley Simulation Results NO BUBBLES 15

10.0um Line/10.0um Space Array AFM Plot of Surface Topography 198nm Peak- Valley Simulation Results NO BUBBLES 16

UW Simulation Results Simulations agree with wafer inspection results in showing no topography bubble defects. All the simulations done with realistic contact angles and corner rounding show No topography bubble entrapment. Does this mean we are safe or are we just not looking at the right conditions? - Topography Type - Defect Mechanism - Other variable 17

Next Steps ISMT-IMEC joint project to more thoroughly test for topography related defects. Topography Reticle/Wafer: - Very wide range of topography (1D, 2D, H&V, BF&DF) - Trench depth, side wall angle, surface contact angle - Optimized for high contrast defect inspection Second level metrology reticle: - Dose sensitive structures covering the entire field. Optimize the resist process flow to achieve a low level of background defects, and do dry exposures for comparisons. 18

Next Step Topography Reticle 1um Label Ynm Xnm 1 2 3 4 5 6 7 8 110um Line Space XXXXXL YYYYYS 1 L/S V PADA LF PAD A DF L BAR Check PAD A DF PADA LF L/S H 29x29 Cell Array 100um Single Cell 10um 2 L BAR DRAM V L/S H Pad B BF DRAM V Pad A Small 45 L/S L BAR 1um Label 3 Check Pad B DF DRAM H Misc Pad B DF Misc Check Pad B BF 4 L/S V PADA LF PAD A DF L BAR Check PAD A DF PADA LF L/S H 5 L/S Small L BAR Small Check Pad B DF 45 L/S L/S V DRAM H L/S Small 110um XXX W YY D 6 Pad B BF Misc L BAR Misc Check L BAR L BAR Small Check 100um 1um 10um Label 7 L BAR Check 45 L/S Pad B BF Pad A Small Pad B DF 45 L/S L BAR 8 L/S V PADA LF PAD A DF L BAR Check PAD A DF PADA LF L/S H 9 110um XXX L YYY VP B 10 2nd L/S V 2nd LF 2nd DF 2nd LF 2nd DF 2n L/S H 100um 10um 1um Label Pad W 110um Space XXXXXW YYYYYS B 100um 10um 19

µ ~90 m Second Level Metrology Reticle 1 2 3 4 5 6 7 8 1 H100 V100 H80 100 L BAR V100 V80 H100 V100 LABEL LABEL LABEL 2 100 L BAR H100 V100 H80 H100 V100 H80 100 L BAR 3 V100 V80 V100 V80 V100 H100 V100 H100 4 H100 H100 H80 100 L BAR H100 V80 H100 V100 5 V100 100 L BAR V100 H100 V100 H100 V100 H100 Cr continues Cr continues 6 H100 H80 100 L BAR V100 H100 100 L BAR H100 V100 LABEL LABEL LABEL 7 100 L BAR H100 V80 H100 V100 100 L BAR V100 100 L BAR 8 H100 V100 H80 ID 100 L BAR H100 V80 H100 V100 9 V100 H100 V100 H100 V100 H100 V100 V80 10 H80 V80 H100 V100 H100 V100 H80 V100 100nm/100nm & 80nm/80nm H & V Line/Space Gratings First immersion exposures with this reticle set in Nov 04. 20

Summary / Conclusions No evidence of topography caused bubble defects. - Limited set of line/space geometry - At defect detectability > 400nm The UW simulations concur with this finding and have shown no bubble formation on any realistic topography. Are we looking at the right conditions? - Topography type - Defect size - Other variable 21

Summary / Conclusions New Topography Reticle/Wafer Developed - Very wide range of topography - Optimized for defect inspection - First immersion exposures in Nov 04 It will be difficult to fully answer defect questions until an immersion tool is installed at a facility with a clean process, available defect metrology, and lots of exposure time (statistics). 22

Intel: Malcolm Delaney, John Urata Acknowledgments ISMT: Chris Van Peski, Rich Berger, Andrew Grenville, Greg Wells IMEC: Young-Chang Kim ASML: Wil Pijnenburg, Gerard Van Reijen KLA-Tencor: Verlyn Fischer, Gian Lorusso Infineon: Nickolay Stepanenko 23