Conventional vs. model-based measurement of patterned line widths from scanning electron microscopy profiles

被引:5
作者
Salvat-Pujol, Francesc [1 ,2 ]
Villarrubia, John S. [1 ]
机构
[1] NIST, Gaithersburg, MD 20899 USA
[2] CERN, CH-1211 Geneva 23, Switzerland
关键词
Critical dimension (CD); Inelastic scattering; JMONSEL; Low-energy electron transport; Nanometer scale dimensional metrology; SEM; Monte Carlo simulation; 41 ELEMENTAL SOLIDS; INELASTIC-SCATTERING; RANGE;
D O I
10.1016/j.ultramic.2019.112819
中图分类号
TH742 [显微镜];
学科分类号
摘要
Scanning electron microscopy (SEM) is a practical tool to determine the dimensions of nanometer-scale features. Conventional width measurements use arbitrary criteria, e.g., a 50 % threshold crossing, to assign feature boundaries in the measured SEM intensity profile. To estimate the errors associated with such a procedure, we have simulated secondary electron signals from a suite of line shapes consisting of 30 nm tall silicon lines with varying width, sidewall angle, and corner rounding. Four different inelastic scattering models were employed in Monte Carlo simulations of electron transport to compute secondary electron image intensity profiles for each of the shapes. The 4 models were combinations of dielectric function theory with either the single-pole approximation (SPA) or the full Penn algorithm (FPA), and either with or without Auger electron emission. Feature widths were determined either by the conventional threshold method or by the model-based library (MBL) method, which is a fit of the simulated profiles to the reference model (FPA + Auger). On the basis of these comparisons we estimate the error in the measured width of such features by the conventional procedure to be as much as several nanometers. A 1 nm difference in the size of, e.g., a nominally 10 nm transistor gate would substantially alter its electronic properties. Thus, the conventional measurements do not meet the contemporary requirements of the semiconductor industry. In contrast, MBL measurements employing models with varying accuracy differed one from another by less than 1 nm. Thus, a MBL measurement is preferable in the nanoscale domain.
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页数:9
相关论文
共 26 条
[1]   Electron spectroscopy imaging and surface defect configuration of zinc oxide nanostructures under different annealing ambient [J].
Ann, Ling Chuo ;
Mahmud, Shahrom ;
Bakhori, Siti Khadijah Mohd .
APPLIED SURFACE SCIENCE, 2013, 265 :137-144
[2]  
[Anonymous], 2002, Algorithms for Minimization Without Derivatives
[3]   Relaxation of an electron system: Conserving approximation [J].
Atwal, GS ;
Ashcroft, NW .
PHYSICAL REVIEW B, 2002, 65 (11) :1-14
[4]  
Fernandez-Varea J.M., 1992, 9206 USIP
[5]   A relativistic optical-data model for inelastic scattering of electrons and positrons in condensed matter [J].
Fernández-Varea, JM ;
Salvat, F ;
Dingfelder, M ;
Lijequist, D .
NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION B-BEAM INTERACTIONS WITH MATERIALS AND ATOMS, 2005, 229 (02) :187-218
[6]   INELASTIC-SCATTERING OF ELECTRONS IN SOLIDS FROM A GENERALIZED OSCILLATOR STRENGTH MODEL USING OPTICAL AND PHOTOELECTRIC DATA [J].
FERNANDEZVAREA, JM ;
MAYOL, R ;
LILJEQUIST, D ;
SALVAT, F .
JOURNAL OF PHYSICS-CONDENSED MATTER, 1993, 5 (22) :3593-3610
[7]   Optical excitations in electron microscopy [J].
Garcia de Abajo, F. J. .
REVIEWS OF MODERN PHYSICS, 2010, 82 (01) :209-275
[8]   Research Update: Electron beam-based metrology after CMOS [J].
Liddle, J. A. ;
Hoskins, B. D. ;
Vladar, A. E. ;
Villarrubia, J. S. .
APL MATERIALS, 2018, 6 (07)
[9]  
LINDHARD J, 1954, MAT FYS MEDD DAN VID, V28, P1
[10]   LINDHARD DIELECTRIC FUNCTION IN RELAXATION-TIME APPROXIMATION [J].
MERMIN, ND .
PHYSICAL REVIEW B-SOLID STATE, 1970, 1 (05) :2362-+