Characterization of Optical Proximity Correction Features

Similar documents
Copyright 2004 by the Society of Photo-Optical Instrumentation Engineers.

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

Copyright 2000 by the Society of Photo-Optical Instrumentation Engineers.

Critical Dimension Uniformity using Reticle Inspection Tool

High Optical Density Photomasks For Large Exposure Applications

Hyper-NA imaging of 45nm node random CH layouts using inverse lithography

The MEEF Shall Inherit the Earth

Copyright 2001 by the Society of Photo-Optical Instrumentation Engineers.

Sensors and Metrology. Outline

Copyright 2001 by the Society of Photo-Optical Instrumentation Engineers.

Chromeless Phase Lithography (CPL)

ADVANCED IMAGING AND OVERLAY PERFORMANCE OF A DUV STEP & SCAN SYSTEM

Methodology of modeling and simulating line-end shortening effects in deep-uv resist

Copyright 1999 by the Society of Photo-Optical Instrumentation Engineers.

= n. Psin. Qualitative Explanation of image degradation by lens + 2. parallel optical beam. θ spatial frequency 1/P. grating with.

Improved Method for Measuring and Assessing Reticle Pinhole Defects for the 100nm Lithography Node

Copyright 2003 by the Society of Photo-Optical Instrumentation Engineers.

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

Bossung Curves; an old technique with a new twist for sub-90 nm nodes Terrence E. Zavecz TEA Systems

IC Fabrication Technology

A Reticle Correction Technique to Minimize Lens Distortion Effects

Chapter 3 : ULSI Manufacturing Technology - (c) Photolithography

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

Photolithography II ( Part 1 )

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

NANO-CMOS DESIGN FOR MANUFACTURABILILTY

Optical Measurements of Critical Dimensions at Several Stages of the Mask Fabrication Process

Story. Cover. An Automated Method for Overlay Sample Plan Optimization

Spectroscopic Critical Dimension technology (SCD) for Directed Self Assembly

Use of Layout Automation and Design Based Metrology for Defect Test Mask Design and Verification

Actinic review of EUV masks: First results from the AIMS EUV system integration

Copyright 1999 by the Society of Photo-Optical Instrumentation Engineers.

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

Figure 1 below shows the generic process flow of an LELE method of double patterning.

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

Lawrence Berkeley National Laboratory Lawrence Berkeley National Laboratory

Copyright 2001 by the Society of Photo-Optical Instrumentation Engineers.

Lecture 14 Advanced Photolithography

Nanoimprint Lithography

Line-Edge Roughness and the Impact of Stochastic Processes on Lithography Scaling for Moore s Law

Overlay Aware Interconnect and Timing Variation Modeling for Double Patterning Technology

A Guide to Reticle Design on the Autostep 200 Edward Tang 6/4/04

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

Automatic Classification and Defect Verification Based on Inspection Technology with Lithography Simulation

193 nm STEP AND SCAN LITHOGRAPHY

nmos IC Design Report Module: EEE 112

T h e Y i e l d M a n a g e m e n t C o m p a n y Electrostatic Compatibility in Photolithography An OEM perspective

Fiducial Marks for EUV mask blanks. Jan-Peter Urbach, James Folta, Cindy Larson, P.A. Kearney, and Thomas White

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

Impact of Pellicle on Overlay in Double Patterning Lithography

Comparison of Techniques to Measure the Point Spread Function due to Scatter and Flare in EUV Lithography Systems

Simulation Based Formulation of a Non-Chemically Amplified Resist for 257 nm Laser Mask Fabrication

Reticle intensity based Critical Dimension Uniformity to improve efficiency for DOMA correction in a foundry

Lecture 0: Introduction

We published the text from the next page.

Litho scenario solutions for FinFET SRAM 22nm node

Across-wafer CD Uniformity Enhancement through Control of Multi-zone PEB Profiles

Silicon VLSI Technology. Fundamentals, Practice and Modeling

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

Effects of Chrome Pattern Characteristics on Image Placement due to the Thermomechanical Distortion of Optical Reticles During Exposure

Improving resist resolution and sensitivity via electric-field enhanced postexposure baking

Title: ASML PAS 5500 Job Creation Semiconductor & Microsystems Fabrication Laboratory Revision: D Rev Date: 09/20/2012

Nanostructures Fabrication Methods

Accurate and Reliable Optical CD of MuGFET down to 10nm

Double patterning for 32nm and below: an update. Jo Finders, Mircea Dusa, Bert Vleeming, Birgitt Hepp, Henry Megens ASML

An analysis of double exposure lithography options

EUV Lithography Towards Industrialization

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

Pattern Collapse. T h e L i t h o g r a p h y E x p e r t (November 2006) Chris A. Mack, Austin, Texas

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

Technology Choices, Challenges and Timing Requirements for Nanolithography at the 32nm Node and Beyond

INTERNATIONAL TECHNOLOGY ROADMAP SEMICONDUCTORS 2001 EDITION METROLOGY FOR

Title: ASML Stepper Semiconductor & Microsystems Fabrication Laboratory Revision: B Rev Date: 12/21/2010

Electron-beam SAFIER process and its application for magnetic thin-film heads

Visual Test Light Scattering Reticle. Users Guide

* AIT-4: Aberrations. Copyright 2006, Regents of University of California

Lithographic Effects Of Acid Diffusion In Chemically Amplified Resists

Feature Profile Evolution during Shallow Trench Isolation (STI) Etch in Chlorine-based Plasmas

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

157nm Lithography with High Numerical Aperture Lens for the 70nm Technology Node

Sensors and Metrology

Optimized Stepping for Fan-out Wafer and Panel Packaging P.10

EUVL Readiness for High Volume Manufacturing

Negative Tone Development: Gaining insight through physical simulation

EE 5211 Analog Integrated Circuit Design. Hua Tang Fall 2012

A Parameter Extraction Framework for DUV Lithography Simulation

Micro- and Nano-Technology... for Optics

Single Pass Die to Database Tritone Reticle Inspection Capability

Behavior of candidate organic pellicle materials under 157 nm laser irradiation

Discussions start next week Labs start in week 3 Homework #1 is due next Friday

More on Stochastics and the Phenomenon of Line-Edge Roughness

Double patterning for 32nm and below: an update. ASML US Inc, 4211 Burton Dr. Santa Clara, CA, USA. IMEC vzw, Kapeldreef 75, B-3001 Heverlee, Belgium;

EE141- Spring 2003 Lecture 3. Last Lecture

Molecular Electronics For Fun and Profit(?)

Microsystems Technology Laboratories i-stepperthursday, October 27, 2005 / site map / contact

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

ITRS, SEMI and ASTM Guidelines for Semiconductor Ultrapure Water (UPW) Production and the Consequences for UPW Particle Metrology

Dan Smith 2016 EUV Mask Pellicle TWG San Jose CA 21 Feb 2016

STANDARD: SPECIFICATION FOR PROTECTIVE ENCLOSURE AND CARRIER SYSTEMS USED TO TRANSPORT AND STORE ( INCH EUV RETICLES

Lithography Challenges Moore s Law Rising Costs and Challenges of Advanced Patterning

Transcription:

Characterization of Optical Proximity Correction Features John Allgair, Michelle Ivy, Kevin Lucas, John Sturtevant Motorola APRDL, Austin, TX 7871 Richard Elliott, Chris A. Mack, Craig MacNaughton, John Miller, Mike Pochkowski, Moshe Preil, John Robinson and Frank Santos KLA-Tencor Corporation, San Jose, CA 95134 ABSTRACT One-dimensional linewidth alone is an inadequate metric for low-k1 lithography. Critical Dimension metrology and analysis have historically focused on 1-dimensional effects but with low-k1 lithography it has increasingly been found that the process window for acceptable imaging of the full -D structure is more limited than the process window for CDs alone. The shape and area of the feature have become as critical to the proper patterning as the width. The measurement and analysis of Critical Shape Difference (CSD) of patterned features must be an integral part of process development efforts. Adoption of optical proximity correction (OPC) and other Optical Extension Technologies increases the need for understanding specific effects through the pattern transfer process. Sub-resolution features on the mask are intended to compensate the pattern so that the resulting etched features most accurately reflect the designer s intent and provide the optimum device performance. A method for quantifying the Critical Shape Difference between the designer s intent, OPC application, mask preparation, resist exposure and pattern etch has been developed. This work focuses on overlaying features from the various process stages and using CSD to quantify the regions of overlap in order to assess OPC performance. Specific examples will demonstrate the gap in current 1-D analysis techniques. Keywords: SEM image analysis, CD SEM, OPC, image analysis, lithography, CSD 1. Introduction One dimensional feature characterization is inadequate for determining process windows for low-k1 lithography. Effects such as line-end pullback further reduce process windows characterized by width alone. Line-end pullback leads to decreased contact area which increases the contact resistance, ultimately causing increased timing delays and compromising device yield, as illustrated in Figure 1. Although the width of the printed lines is within the specification limits, the line-end pullback makes this an unacceptable two dimensional pattern. Line pullback reduces contact area Contact Conductor As Drawn As Printed

Figure 1. Example of line-end pullback. Figure illustrates line-end pullback as a function of k1 (defocus). The data is based on simulation results presented in previous work. As can be seen, the pullback increases steadily with lower k 1 values, and the situation becomes even worse when defocus is considered. Pullback, nm 18 16 14 1 1 8 6 Defocus=um Defocus=.um Defocus=.3um 4 K1 Value 1.1.97.73.6.48.44.36.5um.4um.3um.5um.um.18um.15um Figure. Pullback versus k1 and defocus Line-end pullback can be corrected using two-dimensional OPC as illustrated in Figure 3. The uncorrected reticle design (solid black line) results in severe line-end pullback at the resist level (light gray). Adding OPC features, such as serifs at the reticle level, can improve the resist image (dark gray), but care must be taken to avoid design rule violations. In this example, we require that the OPC structures do not intrude into the adjacent circuit regions, indicated schematically as the Do Not Touch area". No OPC OPC Not Touch Do!!!! Figure 3. Application of two dimensional OPC to correct line-end pullback The effectiveness of the OPC through the printing process needs to be evaluated as shown in Figure 4. Key comparisons to be made include design to resist pattern to etch pattern and mask layout to actual mask pattern. The particular dimensions of the OPC feature must be optimized to obtain the correct feature length after etch.

Design OPC Mask Resist Etch Figure 4. Pattern transfer process, showing the transformation from design level to final etched features. Intermediate steps (OPC layout and mask pattern) may be significantly different than the starting or ending patterns. Key comparisons are design to resist to final etched pattern and layout (with OPC) to mask patterns. Two dimensional feature characterization is required to determine the effectiveness of OPC for reducing lineend pullback. Overlapping process window analysis is common for accessing the lithography process window for isolated and dense features. This paper will demonstrate how the same technique can be extended to the evaluation of OPC performance. C D 19 18 17 16 15 14 13 1 11 19 18 17 16 15 14 13 1 11 Critical Dimension vs. /Exposure ll&s_x_c Doc: d Untitled1 - - - - -...... Focu C Critical Dimension vs. /Exposure ll&s_y_cd Doc: Untitled1 Width Bossung Curve 17. 18. 19.. 1.. 3. 4. 5. 6. 7. Length Bossung Curve 17. 18. 19.. 1.. 3. 4. 5. 6. 7. Dos 1 Overlapping Process Window F - E.4 1.81 - - - - -...... Focu s Group Doc: ProData used to create overlapping process windows ll&s_x_cd ll&s_y_cd Overlap Figure 5. Schematic illustration of the overlapping process window technique.

. Experimental This work focuses on the characterization of OPC required to print a.18 µm wide by.75 µm long trench. In the baseline case, the feature at the reticle level is simply four times larger (4x) than the desired wafer level pattern. In this case, the baseline reticle pattern is a rectangle.7 µm wide by 3. µm long. Four OPC features were compared to a baseline, uncorrected case. The four test cases are summarized in Figure 6. For the OPC cases, the trench was altered from the original layout by biasing the length of the line, and by adding a hammerhead assist feature to the line ends. The hammerheads were 5 nm wider than the line width with a variable overlap dimension. The experimental design tested assist features with overlaps from near zero to almost 1 micron long, and line end extensions from.1 to.5 microns in length at the reticle level. The four features studied in detail tested very short (.1 µm) to fairly long (.5 µm) line end extensions, and hammerheads of two different lengths (.4 and.55 µm). Overlap Test Case None A B C D Length 3 3 3.3 3.1 3.5 Overlap.4.4.55.55 Length * Dimensions are in microns, as drawn on mask (4X) Figure 6. Four OPC test cases compared to baseline (no OPC) case for.18 x.75 micron trench structure. A test reticle was fabricated using this layout, and measured extensively using a KLA-Tencor 81R CD- SEM to determine how accurately the mask making process replicated the intent of the OPC design. The SEM showed that case A no added length and short hammerhead overlap was practically indistinguishable from the baseline case, and it was dropped from further study. -exposure wafers were shot on a.7 NA DUV stepper with annular illumination using Shipley UV1 photoresist and a film stack of Si rich nitride over polysilicon on thin oxide. The two dimensional process windows were also simulated using Prolith 6 to minimize the number of D wafer measurements required. The simulations were not specifically tuned to match the process or lens parameters. Actual reticle images were used in the simulations to capture the realities of the OPC mask making process. The results presented below will compare the relative predictions from the simulations vs. the actual measured data. Both simulated and measured data were ported to the Klarity ProData process window analysis software with the SEM Image Analysis Module (SIAM) to compute and display the overlapping process windows for both feature length and width. The process window tolerances were set at + 1% for the resist linewidth (+ 18 nm). The definition of the process window for the length is subject to more flexibility. For this study, we set the length tolerance to be very close to the absolute value of the width tolerance, or + nm at the wafer level; this is considerably smaller than + 1% of the feature length. Since line-edge pullback is known to vary more as a function of focus and exposure than line width, we expect that this will be a very demanding specification. 3. Results and Discussion

The baseline and test cases B through D are illustrated in Figure 7. Test case A was not included since it was virtually the same as the baseline. As can be seen in Fig. 7a, the baseline case has no overlapping process window for both length and width. At the best exposure for the line width, the trench length is much too short due to line-end pullback. Only by severely overexposing the feature does the length meet the target dimension, resulting in zero overlap between the length and width process windows. As OPC is added in case B, the two windows move closer together, but still fail to overlap. Case C, with longer hammerheads but less length extension, moves the two windows still closer together, resulting in a very small overlapping process window. Finally, case D- with both longer hammerheads and more length extension- shows that we actually overshot the target; the correct exposure dose for the line width now makes the trench too long. The optimum OPC for this case would clearly be between cases C and D. Dose 4 Baseline Dose 4 Test Case B: 3.3 x.4 3 3 5 5 -.4 -.3 -. -.1..1. Dose Test Case C: 3.1 x.55 4 3 5 -.4 -.3 -. -.1..1. -.4 -.3 -. -.1..1. Dose Test Case D: 3.5 x.55 4 3 5 -.4 -.3 -. -.1..1. Length Width Overlap

Figure 7. Baseline and test cases B to D. In viewing the trends of Figs. 7a-d, we see that as OPC is added more aggressively, not only does the process window for feature length move closer to the same optimum dose as the window for feature width, but the size and shape of the length window change as well. The baseline case, where the trench must be drastically overexposed to meet the target length, actually has the largest process window for feature length, in line with previous studies which show that line-end pullback for trench structures is less variable in the overexposed condition. As the OPC becomes more effective at moving the two windows together, the optimum dose for both length and width converges to a single value as desired, but with the undesired side effect that that the size of the process window for the trench length is significantly reduced. Fig. 8 shows experimental data for the process window overlap for an improved design with OPC corrections midway between designs C and D. The process window overlap is improved, but due to the reduced size of the window for trench length and difference in the curvature of the two windows, it still leaves inadequate margin for exposure variation under production conditions. The overlap is greatly improved if we loosen the tolerance on the length to allow more than + nm variation; the exact value required in production must be determined by the specific design rules. 8 7 6 5 4 3 1 Experimental Data -.4 -.3 -. -.1..1. KT 8 SEM data Figure 8. Overlapping process windows for length and width of an optimized trench structure. The process window for line width is the darker dashed line; for trench length, the lighter dashed line. The overlap is shown as a solid line, which mainly follows the limits of the length window. These observations highlight one of the basic difficulties of implementing any form of reticle enhancement technology; the benefit is never obtained without paying a price, and the number of degrees of freedom that must be optimized expands quickly. In this case, we chose the NA and annular illumination conditions to maximize the process window for the line width, then added OPC to match the process window for trench length to the width window. It is quite possible that different combinations of NA, illumination, and OPC might produce better overlap. Exploring the entire parameter space experimentally would be prohibitive; this is where simulation can be especially valuable in guiding the minimum number of experiments. Comparison of experimental and simulated results shows good qualitative agreement, although the quantitative values for dose differ significantly (Fig. 9). This is not surprising since we did not have model

parameters for the specific chemically amplified resist used in the experiments. We were forced to use resist parameters from an older generation resist, and no effort was made to tune the model to achieve better agreement. Despite this, Fig. 9 shows good agreement for both the shape and relative spacing of the two process windows, as well as the two-dimensional top-down patterns, shown here at best focus. 4 PROLITH Simulation 8 Printed Process Window 3 5 -.4 -.3 -. -.1..1. 6 4 -.4-.3-.-.1..1. Figure 9. Comparison of simulated vs. experimental results for the baseline case (no OPC), showing good qualitative agreement between the shape and relative spacing of the process windows, as well as -dimensional top down profiles. 4. Conclusions Both experimental and simulated results show that OPC can be effective in creating overlapping process windows for multiple metrics of pattern quality, but the task of optimizing the reticle and illumination conditions to achieve the best results for these metrics is much more difficult than for one-dimensional CD control of a single feature type. The combination of simulation and experiments can help study multiple combinations of reticle and exposure parameters in a reasonable amount of time, as well as studying other effects which may not be experimentally accessible, such as sensitivity to reticle CD errors (Mask Error Factor). Automating the analysis and display of overlapping process windows greatly expedites the experimental procedure, and provides the means to incorporate other metrics of OPC pattern quality as well, such as corner rounding, critical shape error, or other metrics currently being defined by industry groups. The actual reticle pattern is a critical element to understanding the pattern transfer process. Especially in the case of small OPC corrections, what the CAD software intends to put on the reticle is not necessarily the same as the structure that actually emerges from the mask making process. Reticle SEM measurements are

critical for characterizing the pattern transfer process and determining the optimum OPC models to apply to product layouts. 5. References "Assessment of a hypothetical roadmap that extends optical lithography through the 7-nm technology node", J. Petersen, M. McCallum, N. Kachwala, R. Socha, J.F. Chen, T. Laidig, B.W. SMith, R. Gordon, C. Mack, Proc. SPIE vol. 46, p. 88 (1998) ".5-um logic manufacturability using practical D optical proximity correction", M. Kling, K. Lucas, A. Reich, B. Roman, H. Chuang, P. Gilbert, W. Grobman, E. Travis, P. Tsui, T. Vuong, J. West, Proc. SPIE vol. 3334, p. 4 (1998) "Process window overlap for posts and lines and spaces: optimization by resist type, optical settings, and mask bias", M. Reilly, K. Kvam, J. Willie, Proc. SPIE vol. 3741, p. 4 (1999) "Data analysis for photolithography", C. Mack, S. Jug, D. Legband, Proc. SPIE vol. 3677, p. 415 (1999) "Design, reticle and wafer OPC manufacturability for.18-um lithography generation", K. Lucas, M. McCallum, B. Falch, D. Russell, Proc. SPIE vol. 3679, p.118 (1999) "Manufacturability of sub-wavelength features using reticle and substrate enhancements", K. Lucas, M. McCallum, M. Kling, J. Maltabes, Proc. SPIE vol. 333, p. 391 (1998) "A study of CD SEM suitability fro CD metrology of modern photomasks", W. Ng, G. Anderson, H. Villa, F. Kalk, Proc. SPIE vol. 3748, p. 585 (1999)