Metrology-characterization and simulation of Line Width Roughness (LWR) Evangelos Gogolides, Vassilios Constantoudis, George Patsis Institute of Microelectronics NCSR "Demokritos" Attiki - Greece (in affiliation with lithographic materials team of P. Argitis) More Moore-Excite Joint meeting, Athens May 12, 2005
Outline LWR metrology-characterization methodology 1. Off line detection of line edges and line widths from top down CD-SEM images 2. Characterization of LWR :The importance of sigma(L) curve 3. LWR and CD variation - LWR descriptors B. Simulation of lithography material and process effects on LWR
SEM image after noise smoothing Intensity profile for a pixel row A. LWR metrology-characterization methodology Off line software for the detection of line edges from top down CD-SEM images middle inner outer threshold Normalized pixel intensity SEM image after noise smoothing Determine the pixel size in nm and the noise smoothing parameters Intensity profile for a pixel row Edge detection algorithm at each pixel row using a threshold value Obtain the line edges of the image (outer,inner or middle) A line edge LER : yi,R(L) of all the edges line width or gate length LWR : δyi of all the lines Line length or gate width For uncorrelated and parallel edges : Patsis GP, Constantoudis V, Tserepi A, et al. Quantification of line-edge roughness of photoresists. I. A comparison between off-line and on-line analysis of top-down scanning electron microscopy images J. VAC SCI TECHNOL B 21 (3): 1008-1018 MAY-JUN 2003
A. LWR metrology-characterization methodology 2. Characterization of LWR: The importance of sigmaLWR(L) curve Why sigmaLWR(L) curve : sigma not a value BUT a function, sigma(L) curve 100 200 300 400 500 50 150 250 350 450 x (pixels) y (pixels) L Parameters for sigma(L) curve determination: 1) sigma(inf): the sigma for the infinite line length 2) LS: sigma-correlation length sigma(LS)=0.9*sigma(inf). For L>Ls the line edges look flat (no correlations) and sigma(L)sigma(inf) 3) α : roughness exponent giving the relative contribution of high frequency roughness to LWR. It is related to fractal dimension d=2-α Constantoudis V, Patsis GP, Tserepi A, et al. Quantification of line-edge roughness of photoresists. II. Scaling and fractal analysis and the best roughness descriptorsJ. VAC SCI TECHNOL B 21 (3): 1019-1026 (2003)
A. LWR metrology-characterization methodology The physical meaning of α, Ls Influence of α, Ls on: a) sigmaLWR(L) curve b) edge morphology 1. Different α, the same sigma, Ls α=0.2 α=0.8 3. Different Ls , the same sigma,α LS=300 LS =600
A. LWR metrology-characterization methodology 3. LWR and CD variation : estimating sigmaLWR(inf) using finite line lengths The key relationship : sigmaLWR 2(inf)= sigmaLWR 2(L)+ CDvariation 2(L)+ rmssigma 2(L) variation of sigmaLWR values sigmaLWR(inf): a line length independent parameter that can be estimated using any line length A new parameter for LWR definition ? Also, A new meaning for α,Ls : control the partition of sigmaLWR(inf) in LWR and CD variation as line length L decreases (L<Ls) See paper 5752-141- V. Constantoudis et al. in Metrology Session of SPIE 2005
B. Simulation of material and process effects on LWR Schematic flowchart of simulator Side LER (Accurate) Front View Top - Down LER in 2D Resist Mask Exposure Molecular structure Deprotected Developer
SIMULATION OF ACID DIFFUSION AND MOLECULAR WEIGHT EFFECTS ON LER
SIMULATION OF ACID DIFFUSION AND MOLECULAR WEIGHT EFFECTS ON LER Side LER (Accurate) Front View Top - Down LER in 2D