NIST has introduced a new standard for dimensional metrology and the calibration of the scanning electron microscope
(SEM) scale identifi ed as Reference Material (RM) 8820. RM 8820 was primarily intended to be used for calibrating the
X and Y scale (or magnifi cation) in SEMs but, can be used for an many other purposes. Essentially, all laboratory microscopes
can be calibrated to this same artifact. The NIST pattern is only one part of a very large array of test structures that
were designed for various dimensional metrology purposes useful to semiconductor production technologies. These and
other purposes, discussed in the presentation, RM 8820 can also be used on/in any other type of microscope, such as optical
and scanning probe microscopes and for scatterometry measurements.
Reference Material 8820 (RM 8820) is a new scanning electron microscope calibration reference material for nanotechnology
and nanomanufacturingtion recently released by NIST. This standard was developed to be used primarily for X and
Y scale (or magnifi cation) calibrations of scanning electron microscopes from less than 10 times magnifi cation to more
than 300 000 times magnifi cation, i.e., from about 10 mm to smaller than 300 nm range instrument fi eld of view (FOV).
This standard is identifi ed as RM 8820. This is a very versatile standard, and it can also be used for calibration and testing
of other type of microscopes, such as optical and scanning probe microscopes. Beyond scale calibration, RM 8820 can be
used for a number of other applications, some of which will be described in this publication.
A new multipurpose instrument calibration standard has been released by NIST. This standard was developed to be used
primarily for X and Y scale (or magnification) calibrations of scanning electron microscopes from less than 10 times magnification to more than 300 000 times magnifi cation, i.e., from about 10 mm to smaller than 300 nm range instrument field of view (FOV). This standard is identifi ed as RM 8820. This is a very versatile standard, and it can also be used for calibration
and testing of other type of microscopes, such as optical and scanning probe microscopes. Beyond scale calibration, RM 8820 can be used for a number of other applications, some of which will be described in this publication.
In 2004, the National Institute of Standards and Technology (NIST) commissioned the Advanced Measurement
Laboratory (AML) - a state-of-the-art, five-wing laboratory complex for leading edge NIST research. The NIST
NanoFab - a 1765 m2 (19,000 ft2) clean room with 743 m2 (8000 ft2) of class 100 space - is the anchor of this facility
and an integral component of the new Center for Nanoscale Science and Technology (CNST) at NIST.
Although the CNST/NanoFab is a nanotechnology research facility with a different strategic focus than a current high
volume semiconductor fab, metrology tools still play an important role in the nanofabrication research conducted here.
Some of the metrology tools available to users of the NanoFab include stylus profiling, scanning electron microscopy
(SEM), and atomic force microscopy (AFM).
Since 2001, NIST has collaborated with SEMATECH to implement a reference measurement system (RMS) using
critical dimension atomic force microscopy (CD-AFM). NIST brought metrology expertise to the table and
SEMATECH provided access to leading edge metrology tools in their clean room facility in Austin. Now, in the newly
launched "clean calibrations" thrust at NIST, we are implementing the reference metrology paradigm on several tools in
the CNST/NanoFab. Initially, we have focused on calibration, monitoring, and uncertainty analysis for a three-tool set
consisting of a stylus profiler, an SEM, and an AFM.
Our larger goal is the development of new and supplemental calibrations and standards that will benefit from the
Class 100 environment available in the NanoFab and offering our customers calibration options that do not require
exposing their samples to less clean environments. Toward this end, we have completed a preliminary evaluation of the
performance of these instruments. The results of these evaluations suggest that the achievable uncertainties are
generally consistent with our measurement goals.
We demonstrate optical critical dimension measurement of lines in silicon grating targets using back focal plane scatterfield icroscopy. In this technique, angle-resolved diffraction signatures are obtained from grating targets by imaging the back focal plane of a brightfield microscope that has been modified to allow selection of the angular distribution and polarization of the incident illumination. The target line profiles, including critical dimension linewidth and sidewall angle, are extracted using a scatterometry method that compares the diffraction signatures to a library of theoretical signatures. Because we use the zero-order component of the diffraction, the target features need not be resolved in order to obtain the line profile. We extracted line profiles from two series of targets with fixed pitch but varying linewidth: a subresolution 300-nm-pitch series, and a resolved 600-nm-pitch series. Linewidths of 131 nm to 139 nm were obtained, with nanometer-level sensitivity to linewidth, and a linear relationship of linewidth obtained from scatterfield microscopy to linewidth measured by scanning electron microscopy was demonstrated. Conventional images can be easily collected on the same microscope, providing a powerful tool for combining imaging metrology with scatterometry for optical critical dimension measurement.
KEYWORDS: Transmission electron microscopy, Calibration, Standards development, Crystals, Electron microscopes, Scanning electron microscopy, Metrology, Silicon, Atomic force microscope, Image resolution
One of the key challenges in critical dimension (CD) metrology is finding suitable calibration standards. Over the last
few years there has been some interest in using features measured with the transmission electron microscope (TEM) as
primary standards for linewidth measurements. This is because some modes of TEM can produce lattice-resolved
images having scale traceability to the SI (Systeme International d'Unites or International System of Units) definition of
length through an atomic lattice constant. As interest in using calibration samples that are closer to the length scales
being measured increases, so will the use of these TEM techniques.
An area where lattice-traceable images produced by TEM has been used as a primary standard is in critical dimension
atomic force microscope (CD-AFM) tip width calibration. Two modes of TEM that produce crystal lattice-traceable
images are high resolution transmission electron microscope (HR-TEM) and high angle annular dark field scanning
transmission electron microscope (HAADF-STEM). HR-TEM produces lattice-traceable images by interference
patterns of the diffracted and transmitted beams rather than the actual atomic columns, while HAADF-STEM produces
direct images of the crystal lattice. The difference in how both of these techniques work could cause subtle variations in
the way feature edges are defined.
In this paper, we present results from width samples measured using HR-TEM and HAADF-STEM. Next we compare
the results with measurements taken from the same location by two different CD-AFMs.
Both of the CD-AFM instruments used for this work have been calibrated using a single crystal critical dimension
reference material (SCCDRM). These standards, developed by the National Institute of Standards and Technology
(NIST) and SEMATECH, used HR-TEM for traceable tip-width calibration. Consequently, the present work and the
previous SCCDRM work provide a mutual cross-check on the traceability of the width calibration. Excellent agreement
was observed.
In this paper we present a unique method of evaluating the angular illumination homogeneity in an optical microscope
using the through-focus focus metric. A plot of the sum of the mean square slope throughout an optical image as the
target moves through the focus is defined as the through-focus focus metric. Using optical simulations we show that the
angular illumination inhomogeneity causes the through-focus focus metric value to proportionately increase at specific
focus positions. Based on this observation, we present an experimental method to measure angular illumination
homogeneity by evaluating the through-focus focus metric values on a grid across the field of view. Using the same
through-focus focus metric, we present a detailed study to measure critical dimensions with nanometer sensitivity with
the aid of simulations.
There are numerous metrology challenges facing photolithography for the 45 nm technology node and beyond in the
areas of critical dimension (CD), overlay and defect metrology. Many of these challenges are identified in the 2005
International Technology Roadmap for Semiconductors (ITRS) [1]. The Lithography and Metrology sections of the
ITRS call for measurement of 45/32/22/18 nm generation linewidth and overlay. Each subsequent technology generation
requires less variation in CD linewidth and overlay control, which results in a continuing need for improved metrology
precision. In addition, there is an increasing need to understand individual edge variation and edge placement errors
relative to the intended design. This is accelerating the need for new methods of CD and overlay measurement, as well
as new target structures. This paper will provide a comprehensive overview of the CD and overlay metrology challenges
for photolithography, taking into account the areas addressed in the 2005 ITRS for the 45 nm technology generation and
beyond.
The National Institute of Standards and Technology (NIST) and The International Sematech Manufacturing Initiative
(ISMI) have been involved in a project to evaluate the accuracy of optical overlay measurements in the presence of
measurement target asymmetries created by typical wafer processing. The ultimate goal of this project is to produce a
method of calibrating optical overlay measurements on typical logic and memory production stacks. A method of
performing accurate CD-SEM and CD-AFM overlay measurements is first presented. These measurements are then
compared to optical overlay measurements of the same structures to assess the accuracy of the optical measurements.
Novel image rotation tests were also performed on these structures to develop a method to decouple errors from
metrology target asymmetries and measurement system optical asymmetries.
We have implemented back focal plane (conoscopic) imaging in an optical microscope that has also been modified to allow selection of the illumination angles and polarization at the sample, and collected back focal plane images of silicon on silicon grating scatterometry targets with varying line widths. Using a slit illumination mask, the zero-order diffraction versus angle for −60° to +60° incident angles at a given polarization was obtained from a single image. By using reference images taken on a flat silicon background, we correct the raw target images for illumination source inhomogeneities and polarization-dependent transmission of the optics, and convert them to reflectance versus angle data for s- and p-polarizations, similar to that obtained from angle-resolved grating scatterometry. As with conventional scatterometry, the target lines need not be resolved for the reflectance signature to show sensitivity to small changes in the grating parameters. For a series of 300 nm pitch targets with line widths from 150 nm to 157 nm, we demonstrate nanometer-level sensitivity to line width with good repeatability, using 546 nm illumination. Additionally, we demonstrate a technique for separating the zero order from higher order diffraction on targets with multiple diffraction orders, allowing collection of both zero and higher order diffraction versus angle from the back focal plane image. As conventional images can be easily collected on the same microscope, the method provides a powerful tool for combining imaging metrology with scatterometry for optical critical dimension measurements in semiconductors.
Recent advances in optical imaging techniques have unveiled new possibilities for optical metrology and optical-based process control measurements of features in the 65 nm node and beyond. In this paper we discuss methods and applications that combine illumination engineering and structured targets which enable sensitivity to nanometer scale changes using optical imaging methods. These methods have been investigated using simulation tools and experimental laboratory apparatus. The simulation results have demonstrated substantial sensitivity to nanometer changes in feature geometry. Similar results have now been observed in the laboratory. In this paper we will show simulation data to motivate the use of low numerical aperture and structured illumination optical configurations. We will also present the basic elements and methods which we are now using in the design of an optical tool specifically designed for these types of measurements. Target configurations which enhance the scattered electromagnetic fields will be shown along with experimental verification of the methodology. The simulation and experimental apparatus is used to explore and optimize target geometry, optical configurations, and illumination structure for applications in both critical dimension and overlay metrology.
The optical image of a structured target, where a particular structure repeats itself several times, varies greatly as it is moved through focus if the spacing between the structures is such that the scattered field from the edges interferes. This condition results in a different and complex optical response compared to that found for structures much farther apart. The complex optical image of a structured target in the proximity region is sensitive to the dimensions of the target and the optical parameters. By appropriately analyzing the through-focus optical image, information can be obtained regarding the target and the optical system. In the present work an array of lines is used as a structured target. Experimental data were obtained using a bright field microscope, and results were simulated using a 'modal diffraction grating model' (also known as a rigorous coupled-wave analysis (RCWA)). The gradient-energy focus-metric method was used to characterize the through-focus optical response. The resultant focus metric signature is sensitive to changes in the line width in the nanometer range, giving it potential for metrology applications and characterization of optical tools.
Optical methods are often thought to lose their effectiveness as a metrology tool beyond the Rayleigh criterion. However, using advanced modeling methods, the conventional resolution limitations encountered in well-defined edge-to-edge measurements using edge thresholds do not apply. In fact, in this paper we present evidence that optics can be used to image and measure features as small as 10 nm in dimension, well below the imaging wavelength. To understand the limits of optical methods we have extensively studied both linewidth and overlay metrology applications. Although overlay applications are usually thought to involve pitch or centerline measurements of features from different process levels, some target designs present optical proximity effects which pose a significant challenge. Likewise, line width measurements require determination of the physical edges and geometry which created that profile. Both types of measurements require model-based analysis to accurately evaluate the data and images. In this paper we explore methods to optimize target geometry, optical configurations, structured illumination, and analysis algorithms with applications in both critical dimension and overlay metrology.
The measurement of line-edge roughness (LER) has recently become a topic of concern in the litho-metrology community and the semiconductor industry as a whole. The Advanced Metrology Advisory Group (AMAG), a council composed of the chief metrologists from the International SEMATECH (ISMT) consortium’s Member Companies and from the National Institute of Standards and Technology (NIST), has a project to investigate LER metrics and to direct the critical dimension scanning electron microscope (CD-SEM) supplier community towards a semiconductor industry-backed, standardized solution for implementation. The 2003 International Technology Roadmap for Semiconductors (ITRS) has included a new definition for roughness. The ITRS envisions root mean square measurements of edge and width roughness. There are other possible metrics, some of which are surveyed here. The ITRS envisions the root mean square measurements restricted to roughness wavelengths falling within a specified process-relevant range and with measurement repeatability better than a specified tolerance. This study addresses the measurement choices required to meet those specifications. An expression for the length of line that must be measured and the spacing of measurement positions along that length is derived. Noise in the image is shown to produce roughness measurement errors that have both random and nonrandom (i.e., bias) components. Measurements are reported on both UV resist and polycrystalline silicon in special test patterns with roughness typical for those materials. These measurements indicate that the sensitivity of a roughness measurement to noise depends importantly both on the choice of edge detection algorithm and the quality of the focus. Measurements are less sensitive to noise when a model-based or sigmoidal fit algorithm is used and when the images are in good focus. Using the measured roughness characteristics for UV resist lines and applying the ITRS requirements for the 90 nm technology node, the derived expression for sampling length and sampling interval implies that a length at least 8 times the node (i.e., 720 nm) must be measured at intervals of 7.5 nm or less.
KEYWORDS: Scanning electron microscopy, Electron beams, Model-based design, Silicon, Dimensional metrology, Statistical modeling, Metrology, Monte Carlo methods, Manufacturing, Semiconducting wafers
The widths of 284 lines in a 193 nm resist were measured by two methods and the results compared. One method was scanning electron microscopy (SEM) of cross-sections. The other was a model-based library (MBL) approach in which top-down CD-SEM line scans of structures are compared to a library of simulated line scans, each one of which corresponds to a well-defined sample structure. Feature edge shapes and locations are determined by matching measured to simulated images. This way of determining critical dimensions makes use of known physics of the interaction of the electron beam with the sample, thereby removing some of the ambiguity in sample edge positions that are assigned by more arbitrary methods. Thus far, MBL has shown promise on polycrystalline silicon samples [Villarrubia et al., Proc. SPIE 4689, pp. 304-312 (2002)]. Resist lines, though important in semiconductor manufacturing, pose a more difficult problem because resist tends to shrink and charge upon electron beam exposure. These phenomena are not well characterized, and hence are difficult to include in the models used to construct libraries. Differences between the techniques had a systematic component of 3.5 nm and a random component of about 5 nm. These differences are an upper bound on measurement errors attributable to resist properties, since they are partly attributable to other causes (e.g,. linewidth roughness).
Two types of overlay targets have been designed and evaluated for the study of optical overlay metrology. They are in-chip and arrayed overlay targets. In-chip targets are three-bar two-level targets designed to be placed in or near the active device area of a chip. They occupy a small area in the range of 5 μm2 to 15 μm2 and have line widths, which are nominally device dimensions. The close proximity of the line features result in strong proximity effects. We have used two well-established theoretical models to simulate and study the effects of proximity on overlay measurements. In this paper, we also present a comparison of optical overlay results with scanning electron microscope measurements. Arrayed targets have also been designed to improve and enhance the optical signal for small critical dimension features. We have also compared theoretical simulations of arrayed targets to experimental results. In these comparisons we observe a significant variation in the location of the best focus image with respect to the features. The through-focus focus-metric we have implemented in the current work to determine the best focus image shows interesting properties with potential applications for line width metrology and process control. Based on simulation results, the focus-metric is sensitive to changes in line width dimensions on the nanometer scale.
The Advanced Metrology Advisory Group (AMAG) is a council composed of the chief CD-metrologists from the International SEMATECH Manufacturing Initiative (ISMI) consortium’s Member Companies and from the National Institute of Standards (NIST). The AMAG wrote and, in 2002, with CD-SEM supplier involvement, updated the “Unified Advanced CD-SEM Specification for Sub-130nm Technology (Version 2002)” to be a living document which outlines the required performance of advanced CD-SEMs for supplier compliance to the 2003 International Technology Roadmap for Semiconductors, and also conveys member companies’ other collective needs to vendors. Through applying this specification during the mid-2003 timeframe, a benchmarking effort of the currently available advanced CD-SEMs has been performed. These results are presented here. The AMAG Unified Specification includes sections outlining the test methodologies, metrics, and wafer-target requirements for each parameter included in the benchmark, and, when applicable, prescribes a target specification compatible with the ITRS and methodologies compatible with the demands of 90nm technology. Parameters to be considered include:
•Precision, Repeatability and Reproducibility
•Accuracy, Apparent Beam Width and Resolution
•Charging and Contamination
•Tool-to-Tool Matching
•Pattern Recognition and Navigation Accuracy
•Throughput
•Instrumentation Outputs
•Tool Automation and Utility
•Precision and Accuracy of Profile Measurement
•Precision and Accuracy of Roughness Measurement.
Previous studies under this same project have been published, with the initial version of the International Sematech Unified Specification in 1998, and multi-supplier benchmarks in 1999 and 2001. The results for the 2003 benchmark will be shown and compared to the ITRS, and composite viewpoints showing these 2003 benchmark results compared to the past results are also shown, demonstrating interesting CD-SEM industry trends.
In semiconductor device manufacturing, critical dimension (CD) metrology provides a measurement for precise line-width control during the lithographic process. Currently scanning electron microscope (SEM) tools are typically used for this measurement, because the resolution requirements for the CD measurements are outside the range of optical microscopes. While CD has been a good feedback control for the lithographic process, line-widths continue to shrink and a more precise measurement of the printed lines is needed. With decreasing line widths, the entire sidewall structure must be monitored for precise process control. Sidewall structure is typically acquired by performing a destructive cross sectioning of the device, which is then imaged with a SEM tool. Since cross sectioning is destructive and slow, this is an undesirable method for testing product wafers and only a small sampling of the wafers can be tested. We have developed a technique in which historical cross section/top down image pairs are used to predict sidewall shape from top down SEM images. Features extracted from a new top down SEM image are used to locate similar top downs within the historical database and the corresponding cross sections in the database are combined to create a sidewall estimate for the new top down. Testing with field test data has shown the feasibility of this approach and that it will allow CD SEM tools to provide cross section estimates with no change in hardware or complex modeling.
KEYWORDS: Line edge roughness, Reticles, Line width roughness, Scanning electron microscopy, Line scan image sensors, Edge roughness, Signal to noise ratio, Binary data, Lithography, Semiconductors
The measurement of line-edge roughness (LER) has recently become a major topic of concern in the litho-metrology community and the semiconductor industry as a whole, as addressed in the 2001 International Technology Roadmap for Semiconductors (ITRS) roadmap. The Advanced Metrology Advisory Group (AMAG, a council composed of the chief metrologists from the International SEMATECH (ISMT) consortium’s Member Companies and from the National Institute of Standards and Technology (NIST) has begun a project to investigate this issue and to direct the critical dimension scanning electron microscope (CD-SEM) supplier community towards a semiconductor industry-backed solution for implementation. The AMAG group has designed and built a 193 nm reticle that includes structures
implementing a number of schemes to intentionally cause line edge roughness of various spatial frequencies and amplitudes. The lithography of these structures is in itself of interest to the litho-metrology community and will be discussed here. These structures, along with several other photolithography process variables, have been used to fabricate a set of features of varying roughness value and structure which span the LER process space of interest. These
references are, in turn, useful for evaluation of LER measurement capability.
Measurements on different CD-SEMs of major suppliers were used to demonstrate the current state of LER measurement. These measurements were compared to roughness determined off-line by analysis of top-down images from these tools. While no official standard measurement algorithm or definition of LER measurement exists, definitions
used in this work are presented and compared in use. Repeatability of the measurements and factors affecting their accuracy were explored, as well as how CD-SEM parameters can affect the measurements.
The Overlay Metrology Advisory Group (OMAG) is a group comprised of technical experts in the field of optical metrology from International SEMATECH Member Companies and the National Institute of Standards and Technology (NIST). This council created a specification for overlay metrology benchmarking which indicates the critical parameters to be addressed in order to comply with the International Technology Roadmap for Semiconductors (ITRS) for the 130-nm technology node. A benchmarking study was completed that compares several of the currently available overlay metrology tools. This paper contains the methodologies for benchmarking overlay metrology tools, a comparison of repeatability, reproducibility, throughput, tool-induced shift (TIS) variability, accuracy, and TIS through focus measurements between the participating tools. The tools were identified to the International SEMATECH Member Companies and the appropriate tool suppliers. The identity of the tools will remain only with these select groups. This paper intends to serve as a reference to the current tools' ability to meet the ITRS Roadmap specifications for the 130-nm technology node.
KEYWORDS: Line edge roughness, Reticles, Line width roughness, Edge roughness, Line scan image sensors, Scanning electron microscopy, Signal to noise ratio, Binary data, Lithography, Metrology
The measurement of line-edge roughness (LER) has recently become a major topic of concern in the litho-metrology community and the semiconductor industry as a whole, as addressed in the 2001 ITRS roadmap. The Advanced Metrology Advisory Group (AMAG, a council composed of the chief CD-metrologists from the International SEMATECH consortium's Member Companies and from the National Institute of Standards and Technology, NIST) has begun a project to investigate this issue and to direct the CD-SEM supplier community towards a semiconductor industry-backed solution for implementation. The AMAG group has designed and built a 193 nm reticle that includes structures implementing a number of schemes to intentionally cause line edge roughness of various spatial frequencies and amplitudes. The lithography of these structures is in itself of interest to the litho-metrology community and will be discussed here. Measurements on different CD-SEMs of major suppliers will be used to comparatively demonstrate the current state of LER measurement. These measurements are compared to roughness determined off-line by analysis of top-down images from these tools. While no official standard measurement algorithm or definition of LER measurement exists, definitions used in this work are presented and compared in use. Repeatability of the measurements and factors affecting their accuracy will be explored, as well as how CD-SEM parameters can effect the measurements.
In this work, an extremely flexible and simple dissolution rate monitor (DRM) based on inexpensive, commercially available, PC card spectrometers has been built that can be used quite robustly in both fab and laboratory environments for measuring the dissolution behavior of photoreist films. The hardware required in order to construct such a simple apparatus has been discussed along with various experimental configurations that are appropriate for different measurement tasks. A multiwavelength interferometric data analysis software (MIDAS) has been developed in this work that can robustly perform both single wavelength and multiwavelength DRM data analysis. The multiwavelength DRM and MIDAS software have been found to be very useful in analyzing a variety of resist film dissolution phenomena including monitoring films possessing dissolution rates exceeding 100 nm/s and studying resist film surface inhibition/acceleration. Another useful application has been to measure swelling in the processing of photoresists and other polymer thin films. The basic approaches and algorithms used for thin film thickness and dissolution rate determination in the MIDAS software are discussed in this paper. Results from the use of the MIDAS software in various applications are presented.
One goal of CD metrology is to monitor lithographic process control and how it relates to post-etch results. At present, in-fab process control for this purpose is achieved through top-down CD measurements. To acquire profile information requires destructive cross-section SEM measurements or time-consuming AFM measurements. To find height and profile information about a resist or etched structure directly on a CD-SEM, techniques using the combination of in-column beam tilt and stereographic imaging have been developed, implemented and improved on the Applied Materials NanoSEM-3D. This work is an extension of results previously published, although the tool used is greatly improved and the target feature stacks more thorough. The column of the NanoSEM-3D is designed to be able to electronically tilt the incident beam at small angles as it approaches the sample, through bending the beam within the column. Two images can be captured of the sidewall of the feature target, one at a smaller tilt angle and one at a larger tilt angle. Through matching common features between these two images, a reconstructed profile can be mathematically generated. A feature height and sidewall angle can be calculated, and general shape information such as top-rounding, footing and undercutting can also be displayed. To benchmark the effectiveness of this new technique, an experiment has been conducted to quantify the repeatability and reproducibility of height and sidewall angle measurements of lines of resist-on-poly and the resulting etched-poly lines, and correlate these to measurements of the these same profiles using XSEM to determine the accuracy of the technique. This study will span a reasonable lithographic process window. We hope to demonstrate the necessary precision and accuracy capability to non-destructively replace some cross-section work. In applying these techniques to a common etch bias problem, we also hope to demonstrate a strong correlation which can be used to directly predict post-etch behavior and serve as a model for other etch processes, work with which XSEM cross-sections have typically been used until now. The profile measurement technique is also applied to other CMOS features such as etched STI trench, resist and etched contact holes, and resist and etched damascene trenches and vias, with calculated tool precisions for feature height and sidewall angle.
Critical dimensions in current and next generation devices are driving the need for tighter overlay registration tolerances and improved overlay metrology tool accuracy and repeatability. Tool matching, performance evaluation, and a move towards closed-loop image placement control all place an increase on the importance of improved accuracy and calibration methodology. In response to these industry needs, the National Institute of Standards and Technology (NIST) is introducing a calibrated overlay wafer standard. There are, however, a number of calibration requirements, which must be addressed when using these standards. These include identification of the best methods for evaluating uncertainties when using traceable, calibration artifacts, proper data acquisition and analysis, and the best calibration strategy.
The Advanced Metrology Advisory Group (AMAG) is a council composed of the chief CD-metrologists from the International SEMATECH consortium's Member Companies and from the National Institute of Standards (NIST). The AMAG wrote and, in 2000, updated the 'Unified Advanced CD-SEM Specification for Sub- 0.18 micrometers Technology to be a living document which outlines the required performance of advanced CD-SEMs for vendor compliance to the International Technology Roadmap for Semiconductors, and also conveys other Member companies' collective needs to vendors. Following this specification, a benchmarking effort of the four currently available advanced CD-SEMs has been performed. This paper presents the result of this effort. Previous studies under this same project have ben published.
The Overlay Metrology Advisory Group (OMAG), which includes representatives from International SEMATECH Member Companies and the National Institute of Standards and Technology, has collaborated to create a unified specification for overlay measurement tools [1]. The methodology and results of an overlay benchmarking comparison of several tools are discussed in this paper. As device technologies shrink below the sub-130nm range, a critical need arises to develop more precise tools to measure overlay. Overlay metrology capability needs to be available for detecting and controlling total device overlay regardless of the source of error. The misregistration measurement uncertainty introduced by the overlay tool can be compared for several systems. A benchmarking study is currently underway and focuses on the existing technique of optical measurement of centerline offsets in different target designs. The critical parameters that the study analyzes include precision, accuracy, throughput, through focus measurements, and recipe portability. Imaging issues such as low contrast targets, across wafer thickness variation, CMP effects, and grainy metal targets can contribute greatly to overlay errors. Several process stacks were designed to incorporate some of these imaging issues and test the limitations of the overlay tools. The same set of wafers and test locations were measured at each supplier site and the results were analyzed. This paper focuses on the methodology used for overlay benchmarking and examples of the results generated with respect to the parameters tested.
KEYWORDS: Semiconducting wafers, Calibration, Etching, Critical dimension metrology, Scanning electron microscopy, Lithography, Line edge roughness, Cadmium, Error analysis, Process control
One goal of CD metrology is to monitor lithographic process control and how it relates to post-etch results. At present, in-fab process control for this purpose is achieved through top-done CD measurements. To acquire profile information requires destructive cross-section SEM measurements or time- consuming atomic force microscope (AFM) measurements. To find height and profile information about a resist or etched structure directly on a CD-SEM, new techniques using the combination of in-column beam tilt and stereo graphic imaging have been developed and implemented on the Applied Materials VeraSEM-3D.
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