Electromagnetic Simulation and Modeling With Applications In Lithography

Electromagnetic Simulation and Modeling with Applications in Lithography by Thomas Vincent Pistor Doctor ofPhilosophy in Electrical Engineering University ofCalifornia at Berkeley Professor Andrew R. Neureuther, Chair This thesis is concerned with methods for calculating scattered fields and aerial images in photolithography. Several improvements to the Finite-Difference Time-Domain code TEMPEST are documented and a vector formulation ofoptical imaging is presented. The implementation ofthis theory is then used to study mask effects in EUV lithography, phase defects in alternating phase shift masks and several other lithography-related applications. The numerics ofTEMPEST including the updating equations, domain excitation, conver gence checking, and boundary conditions are reviewed. The Fourier Boundary Condition that operates on the Fourier components of the electromagnetic field is introduced and shown to be useful as an efficient and accurate model for the EUV multilayer mirror. An overview and performance analysis of the re-parallelization of TEMPEST for running across a Network ofWorkstations (NOW) is presented. A vector model for an optical imaging system that can accommodate the highly obUque plane waves existing in high numerical aperture imaging or inspection is developed. Math ematical models for photomasks are presented and organized by their level ofcomplexity. A study of EUVL masks is undertaken where the effects of absorber thickness, side wall angle, comer roimding, angle of incidence and substrate defects are investigated. Key observations include a degradation of mask depth of focus due to off-axis imaging, a dependence of CD on absorber feature thickness due to interference, and the ability of a shallow mirror defect to interact strongly with a mask feature. Phase defects in alternating phase shift masks are investigated from both printability and inspectability points-of-view. Isotropic wet etching was seen to decrease defect printabil ity. Defects with a pre-wet-etch size larger than 200nm were seen to cause greater than 10%CD variation. In simulation studiesofdefect inspectability annular illuminationwas observed to yield stronger normalized difference signal than circular illumination. Thebreadth of uses forTEMPEST in lithography is demonstrated by overviewing simula tions of pinholes, alignment marks, aberration monitors, reflective notching, and twodimensional phase shift mask topographies. Professor A.R. Neureuther Committee Chairman Dedicated to mypoor mom and dad who think Fm coming home now.

[1]  E. Wolf,et al.  Principles of Optics (7th Ed) , 1999 .

[2]  Michael S. Yeung,et al.  Modeling High Numerical Aperture Optical Lithography , 1988, Advanced Lithography.

[3]  Steven A. Orszag,et al.  Derivation and Simulation of Higher Numerical Aperture Scalar Aerial Images , 1992 .

[4]  Andrew R. Neureuther,et al.  Two-Dimensional Optical Proximity Effects , 1986, Advanced Lithography.

[5]  Thomas V. Pistor,et al.  Modeling oblique incidence effects in photomasks , 2000, Advanced Lithography.

[6]  Andrew R. Neureuther,et al.  Coherence of defect interactions with features in optical imaging , 1987 .

[7]  Robert John Socha,et al.  Design of 200nm, 170nm, 140nm DUV contact sweeper high transmission attenuating phase shift mask through simulation. Part 1 , 1998 .

[8]  Yunfei Deng,et al.  Extreme ultraviolet mask defect simulation: Low-profile defects , 2000 .

[9]  Andrew R. Neureuther,et al.  Rigorous three-dimensional time-domain finite-difference electromagnetic simulation , 1995 .

[10]  Sang Hun Lee Extreme ultraviolet (EUV) holographic metrology for lithography applications , 2000 .

[11]  Thomas V. Pistor,et al.  Simulation of reflective notching with TEMPEST , 1997, Advanced Lithography.

[12]  Andreas C. Cangellaris,et al.  GT-PML: generalized theory of perfectly matched layers and its application to the reflectionless truncation of finite-difference time-domain grids , 1996, 1996 IEEE MTT-S International Microwave Symposium Digest.

[13]  Yuri Granik,et al.  Effects of advanced illumination schemes on design manufacturability and interactions with optical proximity corrections , 2000 .

[14]  Srinivas B. Bollepalli,et al.  Computation of reflected images from extreme ultraviolet masks , 1999, Advanced Lithography.

[15]  Christophe Pierrat,et al.  Exposure characteristics of alternate aperture phase‐shifting masks fabricated using a subtractive process , 1992 .

[16]  Will Conley,et al.  Design of 200nm, 170nm, 140nm DUV contact sweeper high transmission attenuating phase shift mask : Experimental results Part 2 , 1999 .

[17]  Robert L. Higdon,et al.  Numerical absorbing boundary conditions for the wave equation , 1987 .

[18]  A. Neureuther,et al.  Mask topography effects in projection printing of phase-shifting masks , 1994 .

[19]  Steven A. Orszag,et al.  Extending scalar aerial image calculations to higher numerical apertures , 1992 .

[20]  K. K. Mei,et al.  Superabsorption-a method to improve absorbing boundary conditions (electromagnetic waves) , 1992 .

[21]  Qiang Wu,et al.  Optimization of segmented alignment marks for advanced semiconductor fabrication processes , 2001, SPIE Advanced Lithography.

[22]  Konstantinos Adam,et al.  Effects of shifter edge topography on through focus performance , 2001, SPIE Photomask Technology.

[23]  Jean-Pierre Berenger,et al.  A perfectly matched layer for the absorption of electromagnetic waves , 1994 .

[24]  H. Hopkins On the diffraction theory of optical images , 1953, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.

[25]  Peter De Bisschop,et al.  Impact of high-order aberrations on the performance of the aberration monitor , 2000, Advanced Lithography.

[26]  Saša Bajt,et al.  Multilayer reflective coatings for extreme-ultraviolet lithography , 1998, Advanced Lithography.

[27]  Zhijian G. Lu,et al.  Subwavelength alignment mark signal analysis of advanced memory products , 2000, Advanced Lithography.

[28]  Roberto Guerrieri,et al.  Massively parallel algorithms for scattering in optical lithography , 1991, IEEE Trans. Comput. Aided Des. Integr. Circuits Syst..

[29]  Andrew R. Neureuther,et al.  Simplified models for edge transitions in rigorous mask modeling , 2001, SPIE Advanced Lithography.

[30]  Allen Taflove,et al.  Computational Electrodynamics the Finite-Difference Time-Domain Method , 1995 .

[31]  W. Penney,et al.  Quantum Mechanics of Electrons in Crystal Lattices , 1931 .

[32]  A. R. Neureuther,et al.  Propagation effects of partial coherence in optical lithography , 1996 .

[33]  Stephen D. Gedney,et al.  An Anisotropic PML Absorbing Media for the FDTD Simulation of Fields in Lossy and Dispersive Media , 1996 .

[34]  Thomas V. Pistor,et al.  Calculating aerial images from EUV masks , 1999, Advanced Lithography.

[35]  Peter De Bisschop,et al.  Novel aberration monitor for optical lithography , 1999, Advanced Lithography.

[36]  Larry S. Zurbrick,et al.  Evaluation of printability and inspection of phase defects on hidden-shifter alternating phase-shift masks , 2000, Photomask Japan.

[37]  Paul B. Mirkarimi,et al.  Investigating the growth of localized defects in thin films using gold nanospheres , 2000 .

[38]  Konstantinos Adam,et al.  Characterization of phase defects in phase shift masks , 2000 .

[39]  Michael S. Yeung,et al.  Extension of the Hopkins theory of partially coherent imaging to include thin-film interference effects , 1993, Advanced Lithography.

[40]  Eric M. Gullikson,et al.  At-wavelength detection of extreme ultraviolet lithography mask blank defects , 1998 .

[41]  Robert John Socha,et al.  Effect of the partial coherence on reflective notching , 1997, Advanced Lithography.

[42]  C. Pierrat,et al.  Phase-shifting mask topography effects on lithographic image quality , 1993, 1992 International Technical Digest on Electron Devices Meeting.

[43]  S.,et al.  Numerical Solution of Initial Boundary Value Problems Involving Maxwell’s Equations in Isotropic Media , 1966 .

[44]  Yunfei Deng,et al.  Rigorous electromagnetic simulation applied to alignment systems , 2001, SPIE Advanced Lithography.

[45]  Khanh Nguyen,et al.  Effects of absorber topography and multilayer coating defects on reflective masks for soft x-ray/EUV projection lithography , 1993, Advanced Lithography.

[46]  Kenneth A. Goldberg,et al.  Extreme ultraviolet interferometry , 1997 .

[47]  Richard H. Stulen,et al.  Printability of substrate and absorber defects on extreme ultraviolet lithographic masks , 1995 .

[48]  G. Mur Absorbing Boundary Conditions for the Finite-Difference Approximation of the Time-Domain Electromagnetic-Field Equations , 1981, IEEE Transactions on Electromagnetic Compatibility.

[49]  Ronald L. Gordon,et al.  Alternating PSM phase defect printability for 100-nm KrF lithography , 2000, Advanced Lithography.