US20040267397A1 - Optical metrology of structures formed on semiconductor wafer using machine learning systems - Google Patents

Optical metrology of structures formed on semiconductor wafer using machine learning systems Download PDF

Info

Publication number
US20040267397A1
US20040267397A1 US10/608,300 US60830003A US2004267397A1 US 20040267397 A1 US20040267397 A1 US 20040267397A1 US 60830003 A US60830003 A US 60830003A US 2004267397 A1 US2004267397 A1 US 2004267397A1
Authority
US
United States
Prior art keywords
machine learning
learning system
diffraction
diffraction signal
training
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Abandoned
Application number
US10/608,300
Inventor
Srinivas Doddi
Emmanuel Drege
Nickhil Jakatdar
Junwei Bao
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Tokyo Electron Ltd
Original Assignee
TEL Timbre Technologies Inc
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by TEL Timbre Technologies Inc filed Critical TEL Timbre Technologies Inc
Priority to US10/608,300 priority Critical patent/US20040267397A1/en
Assigned to TIMBRE TECHNOLOGIES, INC. reassignment TIMBRE TECHNOLOGIES, INC. ASSIGNMENT OF ASSIGNORS INTEREST (SEE DOCUMENT FOR DETAILS). Assignors: BAO, JUNWEI, DODDI, SRINIVAS, DREGE, EMMANUEL, JAKATDAR, NICKHIL
Priority to PCT/US2004/020682 priority patent/WO2005003911A2/en
Priority to KR1020057024949A priority patent/KR101059427B1/en
Priority to DE112004001001T priority patent/DE112004001001T5/en
Priority to CNB2004800149754A priority patent/CN100418083C/en
Priority to JP2006517724A priority patent/JP4589315B2/en
Publication of US20040267397A1 publication Critical patent/US20040267397A1/en
Priority to US12/399,011 priority patent/US7831528B2/en
Assigned to TOKYO ELECTRON LIMITED reassignment TOKYO ELECTRON LIMITED ASSIGNMENT OF ASSIGNORS INTEREST (SEE DOCUMENT FOR DETAILS). Assignors: TIMBRE TECHNOLOGIES, INC.
Abandoned legal-status Critical Current

Links

Images

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01BMEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
    • G01B11/00Measuring arrangements characterised by the use of optical techniques
    • G01B11/24Measuring arrangements characterised by the use of optical techniques for measuring contours or curvatures
    • GPHYSICS
    • G06COMPUTING; CALCULATING OR COUNTING
    • G06NCOMPUTING ARRANGEMENTS BASED ON SPECIFIC COMPUTATIONAL MODELS
    • G06N20/00Machine learning
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L22/00Testing or measuring during manufacture or treatment; Reliability measurements, i.e. testing of parts without further processing to modify the parts as such; Structural arrangements therefor

Definitions

  • the present invention relates to metrology of structures formed on semiconductor wafers, and more particularly to metrology of structures formed on semiconductor wafers using machine learning systems.
  • Optical metrology involves directing an incident beam at a structure, measuring the resulting diffracted beam, and analyzing the diffracted beam to determine a feature of the structure.
  • optical metrology is typically used for quality assurance. For example, after fabricating a periodic grating in proximity to a semiconductor chip on a semiconductor wafer, an optical metrology system is used to determine the profile of the periodic grating. By determining the profile of the periodic grating, the quality of the fabrication process utilized to form the periodic grating, and by extension the semiconductor chip proximate the periodic grating, can be evaluated.
  • One conventional optical metrology system uses a diffraction modeling technique, such as rigorous coupled wave analysis (RCWA), to analyze the diffracted beam. More particularly, in the diffraction modeling technique, a model diffraction signal is calculated based, in part, on solving Maxwell's equations. Calculating the model diffraction signal involves performing a large number of complex calculations, which can be time consuming and costly.
  • RCWA rigorous coupled wave analysis
  • a structure formed on a semiconductor wafer is examined by obtaining a first diffraction signal measured using a metrology device.
  • a second diffraction signal is generated using a machine learning system, where the machine learning system receives as an input one or more parameters that characterize a profile of the structure to generate the second diffraction signal.
  • the first and second diffraction signals are compared.
  • a feature of the structure is determined based on the one or more parameters or the profile used by the machine learning system to generate the second diffraction signal.
  • FIG. 1 depicts an exemplary optical metrology system
  • FIGS. 2A-2E depict exemplary profiles
  • FIG. 3 depicts an exemplary neural network
  • FIG. 4 depicts an exemplary process of training a machine learning system
  • FIG. 5 depicts an exemplary process of testing a machine learning system
  • FIG. 6 depicts an exemplary process of determining a feature of a structure using a machine learning system
  • FIG. 7 depicts an exemplary process of determining a feature of a structure using a machine learning system in a library-based process
  • FIG. 8 depicts an exemplary system to determine a feature of a structure using a machine learning system in a library-based system
  • FIG. 9 depicts an exemplary process of determining a feature of a structure using a machine learning system in a regression-based process
  • FIG. 10 depicts an exemplary system to determine a feature of a structure using a machine learning system in a regression-based system.
  • a metrology system 100 can be used to examine and analyze a structure.
  • metrology system 100 can be used to determine a feature of a periodic grating 102 formed on wafer 104 .
  • periodic grating 102 can be formed in test areas on wafer 104 , such as adjacent to a device formed on wafer 104 .
  • periodic grating 102 can be formed in an area of the device that does not interfere with the operation of the device or along scribe lines on wafer 104 .
  • metrology system 100 can include a metrology device with a source 106 and a detector 112 .
  • Periodic grating 102 is illuminated by an incident beam 108 from source 106 .
  • incident beam 108 is directed onto periodic grating 102 at an angle of incidence ⁇ i with respect to normal n of periodic grating 102 and an azimuth angle ⁇ (i.e., the angle between the plane of incidence beam 108 and the direction of the periodicity of periodic grating 102 ).
  • Diffracted beam 110 leaves at an angle of ⁇ d with respect to normal ⁇ right arrow over (n) ⁇ and is received by detector 112 .
  • Detector 112 converts the diffracted beam 110 into a measured diffraction signal, which can include reflectance, tan ( ⁇ ), cos ( ⁇ ), Fourier coefficients, and the like.
  • Metrology system 100 also includes a processing module 114 configured to receive the measured diffraction signal and analyze the measured diffraction signal. As described below, a feature of periodic grating 102 can then be determined using a library-based process or a regression-based process. Additionally, other linear or non-linear profile extraction techniques are contemplated.
  • the measured diffraction signal is compared to a library of diffraction signals. More specifically, each diffraction signal in the library is associated with a profile of the structure.
  • each diffraction signal in the library is associated with a profile of the structure.
  • the profile associated with the matching diffraction signal in the library is presumed to represent the actual profile of the structure.
  • a feature of the structure can then be determined based on the profile associated with the matching diffraction signal.
  • processing module 114 compares the measured diffraction signal to diffraction signals stored in a library 116 .
  • Each diffraction signal in library 116 is associated with a profile.
  • the profile associated with the matching diffraction signal in library 116 can be presumed to represent the actual profile of periodic grating 102 .
  • the set of profiles stored in library 116 can be generated by characterizing a profile using a set of parameters, then varying the set of parameters to generate profiles of varying shapes and dimensions.
  • the process of characterizing a profile using a set of parameters can be referred to as parameterizing.
  • profile 200 can be characterized by parameters h1 and w1 that define its height and width, respectively.
  • additional shapes and features of profile 200 can be characterized by increasing the number of parameters.
  • profile 200 can be characterized by parameters h1, w1, and w2 that define its height, bottom width, and top width, respectively.
  • the width of profile 200 can be referred to as the critical dimension (CD).
  • parameter w1 and w2 can be described as defining the bottom CD and top CD, respectively, of profile 200 .
  • various types of parameters can be used to characterize profile 200 , including angle of incident (AOI), pitch, n & k, hardware parameters (e.g., polarizer angle), and the like.
  • the set of profiles stored in library 116 can be generated by varying the parameters that characterize the profile. For example, with reference to FIG. 2B, by varying parameters h1, w1, and w2, profiles of varying shapes and dimensions can be generated. Note that one, two, or all three parameters can be varied relative to one another.
  • the parameters of the profile associated with a matching diffraction signal can be used to determine a feature of the structure being examined.
  • a parameter of the profile corresponding to a bottom CD can be used to determine the bottom CD of the structure being examined.
  • the number of profiles and corresponding diffraction signals in the set of profiles and diffraction signals stored in library 116 depends, in part, on the range over which the set of parameters and the increment at which the set of parameters are varied.
  • the profiles and the diffraction signals stored in library 116 are generated prior to obtaining a measured diffraction signal from an actual structure.
  • the range and increment (i.e., the range and resolution) used in generating library 116 can be selected based on familiarity with the fabrication process for a structure and what the range of variance is likely to be.
  • the range and/or resolution of library 116 can also be selected based on empirical measures, such as measurements using atomic force microscopy (AFM), scanning electron microscopy (SEM), and the like.
  • the measured diffraction signal is compared to a diffraction signal generated prior to the comparison (i.e., a trial diffraction signal) using a set of parameters (i.e., trial parameters) for a profile. If the measured diffraction signal and the trial diffraction signal do not match or when the difference of the measured diffraction signal and the trial diffraction signal is not within a preset or matching criterion, another trial diffraction signal is generated using another set of parameters for another profile, then the measured diffraction signal and the newly generated trial diffraction signal are compared.
  • a diffraction signal generated prior to the comparison i.e., a trial diffraction signal
  • trial parameters i.e., trial parameters
  • the profile associated with the matching trial diffraction signal is presumed to represent the actual profile of the structure.
  • the profile associated with the matching trail diffraction signal can then be used to determine a feature of the structure being examined.
  • processing module 114 can generate a trial diffraction signal for a profile, and then compare the measured diffraction signal to the trial diffraction signal. As described above, if the measured diffraction signal and the trial diffraction signal do not match or when the difference of the measured diffraction signal the trial diffraction signals is not within a preset or matching criterion, then processing module 114 can iteratively generate another trial diffraction signal for another profile.
  • the subsequently generated trial diffraction signal can be generated using an optimization algorithm, such as global optimization techniques, which includes simulated annealing, and local optimization techniques, which includes steepest descent algorithm.
  • the trial diffraction signals and profiles can be stored in a library 116 (i.e., a dynamic library).
  • the trial diffraction signals and profiles stored in library 116 can then be subsequently used in matching the measured diffraction signal.
  • library 116 can be omitted from metrology system 100 .
  • diffraction signals used in a library-based process and/or a regression-based process are generated using a machine learning system 118 employing a machine learning algorithm, such as back-propagation, radial basis function, support vector, kernel regression, and the like.
  • a machine learning algorithm such as back-propagation, radial basis function, support vector, kernel regression, and the like.
  • machine learning system 118 receives a profile as an input and generates a diffraction signal as an output.
  • machine learning system 118 is depicted as a component of processing module 114 , it should be recognized that machine learning system 118 can be a separate module.
  • the diffraction signals in library 116 can be generated in advance by machine learning system 118 .
  • machine learning system 118 can be a separate module that is not connected to processing module 114 .
  • machine learning system 118 is used as part of a regression-based process, machine learning system 118 is connected to processing module 114 even when machine learning system 118 is a separate module rather than a component of processing module 114 .
  • the machine learning system is a neural network 300 using a back-propagation algorithm.
  • Neural network 300 includes an input layer 302 , an output layer 304 , and a hidden layer 306 between input layer 302 and output layer 304 .
  • Input layer 302 and hidden layer 306 are connected using links 308 .
  • Hidden layer 306 and output layer 304 are connected using links 310 . It should be recognized, however, that neural network 300 can include any number of layers connected in various configurations.
  • input layer 302 includes one or more input nodes 312 .
  • an input node 312 in input layer 302 corresponds to a parameter of the profile that is inputted into neural network 300 .
  • the number of input nodes 312 corresponds to the number of parameters used to characterize the profile. For example, if a profile is characterized using 2 parameters (e.g., top and bottom widths), input layer 302 includes 2 input nodes 312 , where a first input node 312 corresponds to a first parameter (e.g., a top width) and a second input node 312 corresponds to a second parameter (e.g., a bottom width).
  • output layer 304 includes one or more output nodes 314 .
  • each output node 314 is a linear function. It should be recognized, however, that each output node 314 can be various types of functions.
  • an output node 314 in output layer 304 corresponds to a dimension of the diffraction signal that is outputted from neural network 300 .
  • the number of output nodes 314 corresponds to the number of dimensions used to characterize the diffraction signal.
  • output layer 304 includes 5 output nodes 314 , wherein a first output node 314 corresponds to a first dimension (e.g., a first wavelength), a second output node 314 corresponds to a second dimension (e.g., a second wavelength), etc.
  • a first output node 314 corresponds to a first dimension (e.g., a first wavelength)
  • a second output node 314 corresponds to a second dimension (e.g., a second wavelength)
  • hidden layer 306 includes one or more hidden nodes 316 .
  • each hidden node 316 is a sigmoidal transfer function or a radial basis function. It should be recognized, however, that each hidden node 316 can be various types of functions.
  • the machine learning system Prior to using a machine learning system to generate a diffraction signal, the machine learning system is trained. With reference to FIG. 4, an exemplary process 400 is depicted for training a machine learning system.
  • the machine learning system is trained using a set of training input data and a set of training output data, where an input data in the set of training input data has a corresponding output data in the set of training output data to form an input and an output data pair.
  • the set of training input data is obtained.
  • the training input data includes a set of profiles.
  • a profile is characterized using a set of parameters.
  • a range of profiles can be generated by varying one or more parameters that characterize a profile, either alone or in combination.
  • An overall range of profiles to be generated is determined based on the expected range of variability in the actual profile of the structure to be examined, which is determined either empirically or through experience. For example, if the actual profile of the structure to be examined is expected to have a bottom width that can vary between x 1 and x 2 , then the overall range of profiles can be generated by varying the parameter corresponding to the bottom width between x 1 and x 2 .
  • the set of profiles used to train the machine learning system is selected from the overall range of profiles to be generated. More particularly, the training data set is selected using a random sampling of the overall range of profiles. It should be recognized that various sampling techniques can be used to select the training data set, such as systematic sampling, a combination of random and systematic sampling, and the like.
  • the overall range of profiles to be generated is divided into two or more partitions.
  • a machine learning system is configured and trained for each of the partitions. For example, assume the overall range is divided into a first partition and a second partition. Thus, in this example, a first machine learning system is configured and trained for the first partition, and a second machine learning system is configured and trained for the second partition.
  • One advantage of partitioning the overall range and using multiple machine learning systems is that parallel processing can be used (e.g., the two machine learning systems can be trained and used in parallel).
  • Another advantage is that each of the machine learning systems may be more accurate as to their respective partitions than a single machine learning system for the overall range. More specifically, a single machine learning system trained for the overall range may be susceptible to a local minimum that may reduce the accuracy of the machine learning system.
  • the partitions may be of equal sizes or of varying sizes.
  • the sizes of the partitions can be determined based on the density of the data within the partitions. For example, a less dense partition may be larger than a more dense partition. It should be recognized that the number and size of the partitions can vary depending on the application.
  • the set of training output data is obtained.
  • the training output data includes a set of diffraction signals.
  • a diffraction signal in the set of diffraction signals used as the training output data corresponds to a profile in the set of profiles used as the training input data.
  • Each diffraction signal in the set of diffraction signals can be generated based on each profile in the set of profiles using a modeling technique, such as rigorous coupled wave analysis (RCWA), integral method, Fresnel method, finite analysis, modal analysis, and the like.
  • RCWA rigorous coupled wave analysis
  • each diffraction signal in the set of diffraction signals can be generated based on each profile in the set of profiles using an empirical technique, such as measuring a diffraction signal using a metrology device, such as an ellipsometer, reflectometer, atomic force microscope (AFM), scanning electron microscope (SEM), and the like.
  • a metrology device such as an ellipsometer, reflectometer, atomic force microscope (AFM), scanning electron microscope (SEM), and the like.
  • the set of diffraction signals is transformed using principal component analysis (PCA). More particularly, a diffraction signal can be characterized using a number of dimensions, such as a number of different wavelengths.
  • PCA principal component analysis
  • the diffraction signals are transformed into uncorrelated dimensions, and the space of the uncorrelated dimensions is smaller than the space of the original dimensions. After the machine learning system has been trained, the diffraction signals can be transformed back.
  • the dimensions of the diffraction signals can be divided into two or more partitions.
  • a machine learning system is configured and trained for each of the partitions. For example, assume the dimensions are divided into a first partition and a second partition. Thus, in this example, a first machine learning system is configured and trained for the first partition, and a second machine learning system is configured and trained for the second partition.
  • partitioning the dimensions and using multiple machine learning systems is that parallel processing can be used (e.g., the two machine learning systems can be trained and used in parallel).
  • Another advantage is that each of the machine learning systems may be more accurate as to their respective partitions than a single machine learning system.
  • a diffraction signal is generated using the machine learning system.
  • the generated diffraction signal is compared with the diffraction signal from the set of diffraction signals that corresponds to the profile.
  • 406 and 408 are repeated with another profile from the set of profiles used as the training input data.
  • the training process is terminated.
  • training process 400 can include the use of an optimization technique, such as gradient descent, linear programming, quadratic programming, simulated annealing, Marquardt-Levenberg algorithm, and the like. Additionally, training process 400 can be performed as a batch process. For a more detailed description of a batch process, see “Neural Networks” by Simon Haykin, which has been cited above.
  • training process 400 depicted in FIG. 4 illustrates a back-propagation algorithm.
  • various training algorithms can be used, such as radial basis network, support vector, kernel regression, and the like.
  • an exemplary process 500 is depicted for testing a machine learning system.
  • the machine learning system can be tested to confirm that it has been properly trained. It should be recognized, however, that this testing process can be omitted in some applications.
  • a set of testing input data is obtained.
  • a set of testing output data is obtained.
  • the testing input data includes a set of profiles, and the testing output data includes a set of diffraction signals.
  • the set of testing input data and set of testing output data can be obtained using the same process and techniques described above during the training process.
  • the set of testing input data and set of testing output data can be the same as or a subset of the training input data and training output data.
  • the set of testing input data and set of testing out data can be different than the training input data and training output data.
  • a diffraction signal is generated using the machine learning system.
  • the generated diffraction signal is compared with the diffraction signal from the set of diffraction signals in the testing output data that corresponds to the profile.
  • the machine learning system is re-trained.
  • the training process can be adjusted. For example, the selection and number of the training input and output variables can be adjusted. Additionally, the machine learning system can be adjusted. For example, when the machine learning system is a neural network, as described above, the number of hidden nodes can be adjusted.
  • the testing process is terminated.
  • ERM empirical risk minimization
  • the machine learning system can be used to generate diffraction signals for use in analyzing a structure formed on a semiconductor wafer. Again, it should be noted that the testing process can be omitted in some applications.
  • an exemplary process 600 is depicted for using a machine learning system to examine a structure formed on a semiconductor wafer.
  • a measured diffraction signal of the structure is obtained by using a metrology device.
  • a generated diffraction signal is obtained using the machine learning system.
  • the diffraction signals are compared.
  • a feature of the structure is determined based on the comparison of the measured and generated diffraction signals.
  • a profile corresponding to the generated diffraction signal is used as an input to the machine learning system to generate the generated diffraction signal.
  • the profile is characterized by one or more parameters.
  • an exemplary process 700 is depicted for using a machine learning system in a library-based process.
  • a library of diffraction signals are generated using the machine learning system. More particularly, the library of diffraction signals is generated by inputting a range of profiles into the machine learning system.
  • a measured diffraction signal is obtained using a metrology device, such as an ellipsometer, reflectometer, and the like.
  • the measured diffraction signal is compared to the diffraction signals in the library of diffraction signals generated using the machine learning system.
  • a feature of the structure is determined using the profile corresponding to the matching diffraction signal from the library of diffraction signals.
  • an exemplary system 800 is depicted for using a machine learning system in a library-based system.
  • library 116 is generated using machine learning system 118 .
  • Library 116 is then used by processing module 114 to compare the diffraction signals in library 116 to measured diffraction signals obtained from a metrology device 802 , such as an ellipsometer, a reflectometer, and the like.
  • a metrology device 802 such as an ellipsometer, a reflectometer, and the like.
  • machine learning system 118 is depicted as a separate unit in FIG. 8, machine learning system 118 can be integrated as a component of processing module 114 .
  • machine learning system 118 can be connected to processing module 114 to transmit library 116 to processing module 114 , such as through a network connection.
  • library 116 can be stored on a portable storage medium and physically transported to processing module 114 .
  • processing module 114 can be coupled to a semiconductor fabrication unit 804 that is configured to perform one or more fabrication steps. It should be recognized, however, that the metrology system can operate as a stand-alone system in addition to being integrated with semiconductor fabrication unit 804 .
  • an exemplary process 900 is depicted for using a machine learning system in a regression-based process.
  • a measured diffraction signal is obtained using a metrology device, such as an ellipsometer, reflectometer, atomic force microscope (AFM), scanning electron microscope (SEM),and the like.
  • a generated diffraction signal is obtained using the machine learning system.
  • the two diffraction signals are compared. When the two diffraction signals do not match within a predetermined matching criterion, 904 and 906 are repeated with another diffraction signal generated in 904 .
  • This process is iterated until a match is found, meaning that the generated and measured diffraction signals match within the predetermined matching criterion.
  • the profile corresponding to the matching diffraction signal is assumed to correspond to the actual profile of the structure being examined.
  • the profile and the parameters that characterize the profile can be used to determine a feature of the structure.
  • an exemplary system 1000 is depicted for using a machine learning system in a regression-based system.
  • an optimizer 1002 receives the measured diffraction signal as an input from metrology device 802 .
  • Optimizer 1002 receives the generated diffraction signal as an input from machine learning system 118 .
  • Optimizer 1002 compares the generated and the measured diffraction signals. When the generated and measured diffraction signals do match, optimizer 1002 outputs the profile corresponding to the matching generated diffraction signal. When the generated and measured diffraction signals do not match within a predetermined matching criterion, optimizer 1002 outputs a signal to machine learning system 118 to generate another diffraction signal. This process is iterated until a match is found, meaning that the generated and measured diffraction signals match within the predetermined matching criterion.
  • an optimization technique is used to reduce the number of iterations needed to arrive at a match. More particularly, the aim of an optimization problem is to find a best solution among several possible solutions, where the best solution can be quantified by associating a cost function. In other words, for a given problem under a given cost metric, the task is to find a solution with the least cost. Thus, in the present exemplary application, the task is to find the profile with a corresponding diffraction signal that produces the least cost (under a given cost metric) with respect to the given measured diffraction signal.
  • optimization techniques which are broadly classified into two categories (i.e., global and local), are known and can be used, such as gradient descent, linear programming, quadratic programming, simulated annealing, Marquardt-Levenberg algorithm, and the like.
  • global and local optimization techniques see “Numerical Recipes in C”, by William H. Press, Saul A. Teukolsky, William T. Vetterling and Brian P. Flannery, Second Edition, Cambridge, which is incorporated herein by reference.
  • a library of diffraction signals can be generated as part of a regression-based process. More particularly, when a match has been made, meaning that the generated diffraction signal and the measured diffraction signal match within the matching criterion, a library of diffraction signals can be generated around the matching profile. Generally, the library of diffraction signals generated as part of the regression-based process is smaller than the library that is generated as part of the library-based process described above.
  • the library of diffraction signals generated as part of a regression-based process and the library generated as part of a library-based process described above can be used in an interpolation process, where a solution is derived between two entries in the library.
  • an interpolation process see U.S. patent application Ser. No. 10/075,904, titled PROFILE REFINEMENT FOR INTEGRATED CIRCUIT METROLOGY, filed on Feb. 12, 2002, which is incorporated herein by reference in its entirety.
  • machine learning system 118 can be configured to operate with a non-optical metrology device, such as an atomic force microscope (AFM), scanning electron microscopes (SEM), and the like, or a combination of an optical and a non-optical metrology device.
  • a non-optical metrology device such as an atomic force microscope (AFM), scanning electron microscopes (SEM), and the like
  • machine learning system 118 can generate various types of diffraction signals corresponding to the type of metrology device used.
  • the diffraction signal generated by machine learning system 118 is a SEM signal, such as two-dimensional images or SEM traces.
  • the diffraction signal generated can include characteristic functions of the signal used by the metrology device.
  • various order derivatives e.g., first order, second order . . . n th order derivatives
  • Marquardt-Levenberg algorithm to optimize the training process.

Abstract

A structure formed on a semiconductor wafer is examined by obtaining a first diffraction signal measured using a metrology device. A second diffraction signal is generated using a machine learning system, where the machine learning system receives as an input one or more parameters that characterize a profile of the structure to generate the second diffraction signal. The first and second diffraction signals are compared. When the first and second diffraction signals match within a matching criterion, a feature of the structure is determined based on the one or more parameters or the profile used by the machine learning system to generate the second diffraction signal.

Description

    BACKGROUND
  • 1. Field of the Invention [0001]
  • The present invention relates to metrology of structures formed on semiconductor wafers, and more particularly to metrology of structures formed on semiconductor wafers using machine learning systems. [0002]
  • 2. Related Art [0003]
  • Optical metrology involves directing an incident beam at a structure, measuring the resulting diffracted beam, and analyzing the diffracted beam to determine a feature of the structure. In semiconductor manufacturing, optical metrology is typically used for quality assurance. For example, after fabricating a periodic grating in proximity to a semiconductor chip on a semiconductor wafer, an optical metrology system is used to determine the profile of the periodic grating. By determining the profile of the periodic grating, the quality of the fabrication process utilized to form the periodic grating, and by extension the semiconductor chip proximate the periodic grating, can be evaluated. [0004]
  • One conventional optical metrology system uses a diffraction modeling technique, such as rigorous coupled wave analysis (RCWA), to analyze the diffracted beam. More particularly, in the diffraction modeling technique, a model diffraction signal is calculated based, in part, on solving Maxwell's equations. Calculating the model diffraction signal involves performing a large number of complex calculations, which can be time consuming and costly. [0005]
  • SUMMARY
  • In one exemplary embodiment, a structure formed on a semiconductor wafer is examined by obtaining a first diffraction signal measured using a metrology device. A second diffraction signal is generated using a machine learning system, where the machine learning system receives as an input one or more parameters that characterize a profile of the structure to generate the second diffraction signal. The first and second diffraction signals are compared. When the first and second diffraction signals match within a matching criterion, a feature of the structure is determined based on the one or more parameters or the profile used by the machine learning system to generate the second diffraction signal.[0006]
  • DESCRIPTION OF DRAWING FIGURES
  • The present invention can be best understood by reference to the following description taken in conjunction with the accompanying drawing figures, in which like parts may be referred to by like numerals: [0007]
  • FIG. 1 depicts an exemplary optical metrology system; [0008]
  • FIGS. 2A-2E depict exemplary profiles; [0009]
  • FIG. 3 depicts an exemplary neural network; [0010]
  • FIG. 4 depicts an exemplary process of training a machine learning system; [0011]
  • FIG. 5 depicts an exemplary process of testing a machine learning system; [0012]
  • FIG. 6 depicts an exemplary process of determining a feature of a structure using a machine learning system; [0013]
  • FIG. 7 depicts an exemplary process of determining a feature of a structure using a machine learning system in a library-based process; [0014]
  • FIG. 8 depicts an exemplary system to determine a feature of a structure using a machine learning system in a library-based system; [0015]
  • FIG. 9 depicts an exemplary process of determining a feature of a structure using a machine learning system in a regression-based process; and [0016]
  • FIG. 10 depicts an exemplary system to determine a feature of a structure using a machine learning system in a regression-based system.[0017]
  • DETAILED DESCRIPTION
  • The following description sets forth numerous specific configurations, parameters, and the like. It should be recognized, however, that such description is not intended as a limitation on the scope of the present invention, but is instead provided as a description of exemplary embodiments. [0018]
  • 1. Metrology [0019]
  • With reference to FIG. 1, a [0020] metrology system 100 can be used to examine and analyze a structure. For example, metrology system 100 can be used to determine a feature of a periodic grating 102 formed on wafer 104. As described earlier, periodic grating 102 can be formed in test areas on wafer 104, such as adjacent to a device formed on wafer 104. Alternatively, periodic grating 102 can be formed in an area of the device that does not interfere with the operation of the device or along scribe lines on wafer 104.
  • As depicted in FIG. 1, [0021] metrology system 100 can include a metrology device with a source 106 and a detector 112. Periodic grating 102 is illuminated by an incident beam 108 from source 106. In the present exemplary embodiment, incident beam 108 is directed onto periodic grating 102 at an angle of incidence θi with respect to normal n of periodic grating 102 and an azimuth angle Φ (i.e., the angle between the plane of incidence beam 108 and the direction of the periodicity of periodic grating 102). Diffracted beam 110 leaves at an angle of θd with respect to normal {right arrow over (n)} and is received by detector 112. Detector 112 converts the diffracted beam 110 into a measured diffraction signal, which can include reflectance, tan (Ψ), cos (Δ), Fourier coefficients, and the like.
  • [0022] Metrology system 100 also includes a processing module 114 configured to receive the measured diffraction signal and analyze the measured diffraction signal. As described below, a feature of periodic grating 102 can then be determined using a library-based process or a regression-based process. Additionally, other linear or non-linear profile extraction techniques are contemplated.
  • 2. Library-based Process [0023]
  • In a library-based process, the measured diffraction signal is compared to a library of diffraction signals. More specifically, each diffraction signal in the library is associated with a profile of the structure. When a match is made between the measured diffraction signal and one of the diffraction signals in the library or when the difference of the measured diffraction signal and one of the diffraction signals in the library is within a preset or matching criterion, the profile associated with the matching diffraction signal in the library is presumed to represent the actual profile of the structure. A feature of the structure can then be determined based on the profile associated with the matching diffraction signal. [0024]
  • Thus, with reference again to FIG. 1, in one exemplary embodiment, after obtaining a measured diffraction signal, [0025] processing module 114 compares the measured diffraction signal to diffraction signals stored in a library 116. Each diffraction signal in library 116 is associated with a profile. When a match is made between the measured diffraction signal and one of the diffraction signals in library 116, the profile associated with the matching diffraction signal in library 116 can be presumed to represent the actual profile of periodic grating 102.
  • The set of profiles stored in [0026] library 116 can be generated by characterizing a profile using a set of parameters, then varying the set of parameters to generate profiles of varying shapes and dimensions. The process of characterizing a profile using a set of parameters can be referred to as parameterizing.
  • For example, as depicted in FIG. 2A, assume that [0027] profile 200 can be characterized by parameters h1 and w1 that define its height and width, respectively. As depicted in FIGS. 2B to 2E, additional shapes and features of profile 200 can be characterized by increasing the number of parameters. For example, as depicted in FIG. 2B, profile 200 can be characterized by parameters h1, w1, and w2 that define its height, bottom width, and top width, respectively. Note that the width of profile 200 can be referred to as the critical dimension (CD). For example, in FIG. 2B, parameter w1 and w2 can be described as defining the bottom CD and top CD, respectively, of profile 200. It should be recognized that various types of parameters can be used to characterize profile 200, including angle of incident (AOI), pitch, n & k, hardware parameters (e.g., polarizer angle), and the like.
  • As described above, the set of profiles stored in library [0028] 116 (FIG. 1) can be generated by varying the parameters that characterize the profile. For example, with reference to FIG. 2B, by varying parameters h1, w1, and w2, profiles of varying shapes and dimensions can be generated. Note that one, two, or all three parameters can be varied relative to one another.
  • Thus, the parameters of the profile associated with a matching diffraction signal can be used to determine a feature of the structure being examined. For example, a parameter of the profile corresponding to a bottom CD can be used to determine the bottom CD of the structure being examined. [0029]
  • With reference again to FIG. 1, the number of profiles and corresponding diffraction signals in the set of profiles and diffraction signals stored in library [0030] 116 (i.e., the resolution and/or range of library 116) depends, in part, on the range over which the set of parameters and the increment at which the set of parameters are varied. In one exemplary embodiment, the profiles and the diffraction signals stored in library 116 are generated prior to obtaining a measured diffraction signal from an actual structure. Thus, the range and increment (i.e., the range and resolution) used in generating library 116 can be selected based on familiarity with the fabrication process for a structure and what the range of variance is likely to be. The range and/or resolution of library 116 can also be selected based on empirical measures, such as measurements using atomic force microscopy (AFM), scanning electron microscopy (SEM), and the like.
  • For a more detailed description of a library-based process, see U.S. patent application Ser. No. 09/907,488, titled GENERATION OF A LIBRARY OF PERIODIC GRATING DIFFR5TION SIGNALS, filed on Jul. 16, 2001, which is incorporated herein by reference in its entirety. [0031]
  • 3. Regression-based Process [0032]
  • In a regression-based process, the measured diffraction signal is compared to a diffraction signal generated prior to the comparison (i.e., a trial diffraction signal) using a set of parameters (i.e., trial parameters) for a profile. If the measured diffraction signal and the trial diffraction signal do not match or when the difference of the measured diffraction signal and the trial diffraction signal is not within a preset or matching criterion, another trial diffraction signal is generated using another set of parameters for another profile, then the measured diffraction signal and the newly generated trial diffraction signal are compared. When the measured diffraction signal and the trial diffraction signal match or when the difference of the measured diffraction signal and the trial diffraction signals is within a preset or matching criterion, the profile associated with the matching trial diffraction signal is presumed to represent the actual profile of the structure. The profile associated with the matching trail diffraction signal can then be used to determine a feature of the structure being examined. [0033]
  • Thus, with reference again to FIG. 1, in one exemplary embodiment, [0034] processing module 114 can generate a trial diffraction signal for a profile, and then compare the measured diffraction signal to the trial diffraction signal. As described above, if the measured diffraction signal and the trial diffraction signal do not match or when the difference of the measured diffraction signal the trial diffraction signals is not within a preset or matching criterion, then processing module 114 can iteratively generate another trial diffraction signal for another profile. In one exemplary embodiment, the subsequently generated trial diffraction signal can be generated using an optimization algorithm, such as global optimization techniques, which includes simulated annealing, and local optimization techniques, which includes steepest descent algorithm.
  • In one exemplary embodiment, the trial diffraction signals and profiles can be stored in a library [0035] 116 (i.e., a dynamic library). The trial diffraction signals and profiles stored in library 116 can then be subsequently used in matching the measured diffraction signal. Alternatively, library 116 can be omitted from metrology system 100.
  • For a more detailed description of a regression-based process, see U.S. patent application Ser. No. 09/923,578, titled METHOD AND SYSTEM OF DYNAMIC LEARNING THROUGH A REGRESSION-BASED LIBRARY GENERATION PROCESS, filed on Aug. 6, 2001, which is incorporated herein by reference in its entirety. [0036]
  • 4. Machine Learning Systems [0037]
  • With reference to FIG. 1, in one exemplary embodiment, diffraction signals used in a library-based process and/or a regression-based process are generated using a [0038] machine learning system 118 employing a machine learning algorithm, such as back-propagation, radial basis function, support vector, kernel regression, and the like. For a more detailed description of machine learning systems and algorithms, see “Neural Networks” by Simon Haykin, Prentice Hall, 1999, which is incorporated herein by reference in its entirety.
  • In the present exemplary embodiment, [0039] machine learning system 118 receives a profile as an input and generates a diffraction signal as an output. Although in FIG. 1 machine learning system 118 is depicted as a component of processing module 114, it should be recognized that machine learning system 118 can be a separate module. Moreover, when machine learning system 118 is used as part of a library-based process, the diffraction signals in library 116 can be generated in advance by machine learning system 118. As such, machine learning system 118 can be a separate module that is not connected to processing module 114. In contrast, when machine learning system 118 is used as part of a regression-based process, machine learning system 118 is connected to processing module 114 even when machine learning system 118 is a separate module rather than a component of processing module 114.
  • With reference to FIG. 3, in one exemplary implementation, the machine learning system is a [0040] neural network 300 using a back-propagation algorithm. Neural network 300 includes an input layer 302, an output layer 304, and a hidden layer 306 between input layer 302 and output layer 304. Input layer 302 and hidden layer 306 are connected using links 308. Hidden layer 306 and output layer 304 are connected using links 310. It should be recognized, however, that neural network 300 can include any number of layers connected in various configurations.
  • As depicted in FIG. 3, [0041] input layer 302 includes one or more input nodes 312. In the present exemplary implementation, an input node 312 in input layer 302 corresponds to a parameter of the profile that is inputted into neural network 300. Thus, the number of input nodes 312 corresponds to the number of parameters used to characterize the profile. For example, if a profile is characterized using 2 parameters (e.g., top and bottom widths), input layer 302 includes 2 input nodes 312, where a first input node 312 corresponds to a first parameter (e.g., a top width) and a second input node 312 corresponds to a second parameter (e.g., a bottom width).
  • In [0042] neural network 300, output layer 304 includes one or more output nodes 314. In the present exemplary implementation, each output node 314 is a linear function. It should be recognized, however, that each output node 314 can be various types of functions. Additionally, in the present exemplary implementation, an output node 314 in output layer 304 corresponds to a dimension of the diffraction signal that is outputted from neural network 300. Thus, the number of output nodes 314 corresponds to the number of dimensions used to characterize the diffraction signal. For example, if a diffraction signal is characterized using 5 dimensions corresponding to, for example, 5 different wavelengths, output layer 304 includes 5 output nodes 314, wherein a first output node 314 corresponds to a first dimension (e.g., a first wavelength), a second output node 314 corresponds to a second dimension (e.g., a second wavelength), etc.
  • In [0043] neural network 300, hidden layer 306 includes one or more hidden nodes 316. In the present exemplary implementation, each hidden node 316 is a sigmoidal transfer function or a radial basis function. It should be recognized, however, that each hidden node 316 can be various types of functions. Additionally, in the present exemplary implementation, the number of hidden nodes 316 is determined based on the number of output nodes 314. More particularly, the number of hidden nodes 316 (m) is related to the number of output nodes 314 (n) by a predetermined ratio (r=m/n). For example, when r=10, there are 10 hidden nodes 316 for each output node 314. It should be recognized, however, that the predetermined ratio can be a ratio of the number of output nodes 314 to the number of hidden nodes 316 (i.e., r=n/m). Additionally, it should be recognized that the number of hidden nodes 316 in neural network 300 can be adjusted after the initial number of hidden nodes 316 is determined based on the predetermined ratio. Furthermore, the number of hidden nodes 316 in neural network 300 can be determined based on experience and/or experimentation rather than based on the predetermined ratio.
  • Prior to using a machine learning system to generate a diffraction signal, the machine learning system is trained. With reference to FIG. 4, an [0044] exemplary process 400 is depicted for training a machine learning system. In exemplary process 400, the machine learning system is trained using a set of training input data and a set of training output data, where an input data in the set of training input data has a corresponding output data in the set of training output data to form an input and an output data pair.
  • In [0045] 402, the set of training input data is obtained. In the present exemplary embodiment, the training input data includes a set of profiles. As described above, a profile is characterized using a set of parameters. A range of profiles can be generated by varying one or more parameters that characterize a profile, either alone or in combination. An overall range of profiles to be generated is determined based on the expected range of variability in the actual profile of the structure to be examined, which is determined either empirically or through experience. For example, if the actual profile of the structure to be examined is expected to have a bottom width that can vary between x1 and x2, then the overall range of profiles can be generated by varying the parameter corresponding to the bottom width between x1 and x2.
  • In one exemplary implementation, the set of profiles used to train the machine learning system is selected from the overall range of profiles to be generated. More particularly, the training data set is selected using a random sampling of the overall range of profiles. It should be recognized that various sampling techniques can be used to select the training data set, such as systematic sampling, a combination of random and systematic sampling, and the like. [0046]
  • In the present exemplary implementation, the overall range of profiles to be generated is divided into two or more partitions. A machine learning system is configured and trained for each of the partitions. For example, assume the overall range is divided into a first partition and a second partition. Thus, in this example, a first machine learning system is configured and trained for the first partition, and a second machine learning system is configured and trained for the second partition. One advantage of partitioning the overall range and using multiple machine learning systems is that parallel processing can be used (e.g., the two machine learning systems can be trained and used in parallel). Another advantage is that each of the machine learning systems may be more accurate as to their respective partitions than a single machine learning system for the overall range. More specifically, a single machine learning system trained for the overall range may be susceptible to a local minimum that may reduce the accuracy of the machine learning system. [0047]
  • When the overall range is partitioned, the partitions may be of equal sizes or of varying sizes. When the partitions are of varying sizes, the sizes of the partitions can be determined based on the density of the data within the partitions. For example, a less dense partition may be larger than a more dense partition. It should be recognized that the number and size of the partitions can vary depending on the application. [0048]
  • In [0049] 404, the set of training output data is obtained. In the present exemplary embodiment, the training output data includes a set of diffraction signals. A diffraction signal in the set of diffraction signals used as the training output data corresponds to a profile in the set of profiles used as the training input data. Each diffraction signal in the set of diffraction signals can be generated based on each profile in the set of profiles using a modeling technique, such as rigorous coupled wave analysis (RCWA), integral method, Fresnel method, finite analysis, modal analysis, and the like. Alternatively, each diffraction signal in the set of diffraction signals can be generated based on each profile in the set of profiles using an empirical technique, such as measuring a diffraction signal using a metrology device, such as an ellipsometer, reflectometer, atomic force microscope (AFM), scanning electron microscope (SEM), and the like. Thus, a profile from the set of profiles and the corresponding diffraction signal from the set of diffraction signals form a profile/diffraction signal pair. Although there is a one-to-one correspondence between a profile and a diffraction signal in the profile/diffraction signal pair, note that there does not need to be a known relation, either analytic or numeric, between the profile and the diffraction signal in the profile/diffraction signal pair.
  • In one exemplary implementation, prior to using the set of diffraction signals to train the machine learning system, the set of diffraction signals is transformed using principal component analysis (PCA). More particularly, a diffraction signal can be characterized using a number of dimensions, such as a number of different wavelengths. By using PCA to transform the set of diffraction signals, the diffraction signals are transformed into uncorrelated dimensions, and the space of the uncorrelated dimensions is smaller than the space of the original dimensions. After the machine learning system has been trained, the diffraction signals can be transformed back. [0050]
  • In the present exemplary implementation, the dimensions of the diffraction signals can be divided into two or more partitions. A machine learning system is configured and trained for each of the partitions. For example, assume the dimensions are divided into a first partition and a second partition. Thus, in this example, a first machine learning system is configured and trained for the first partition, and a second machine learning system is configured and trained for the second partition. Again, one advantage of partitioning the dimensions and using multiple machine learning systems is that parallel processing can be used (e.g., the two machine learning systems can be trained and used in parallel). Another advantage is that each of the machine learning systems may be more accurate as to their respective partitions than a single machine learning system. [0051]
  • In [0052] 406, for a profile from the set of profiles used as the training input data, a diffraction signal is generated using the machine learning system. In 408, the generated diffraction signal is compared with the diffraction signal from the set of diffraction signals that corresponds to the profile. When the difference between the diffraction signals are not within a desired or predetermined margin of error, 406 and 408 are repeated with another profile from the set of profiles used as the training input data. In 410, when the difference between the diffraction signals are within a desired or predetermined margin of error, the training process is terminated.
  • It should be recognized that [0053] training process 400 can include the use of an optimization technique, such as gradient descent, linear programming, quadratic programming, simulated annealing, Marquardt-Levenberg algorithm, and the like. Additionally, training process 400 can be performed as a batch process. For a more detailed description of a batch process, see “Neural Networks” by Simon Haykin, which has been cited above.
  • Furthermore, [0054] training process 400 depicted in FIG. 4 illustrates a back-propagation algorithm. However, it should be recognized that various training algorithms can be used, such as radial basis network, support vector, kernel regression, and the like.
  • With reference to FIG. 5, an [0055] exemplary process 500 is depicted for testing a machine learning system. In one exemplary embodiment, after a machine learning system has been trained, the machine learning system can be tested to confirm that it has been properly trained. It should be recognized, however, that this testing process can be omitted in some applications.
  • In [0056] 502, a set of testing input data is obtained. In 504, a set of testing output data is obtained. In the present exemplary embodiment, the testing input data includes a set of profiles, and the testing output data includes a set of diffraction signals. The set of testing input data and set of testing output data can be obtained using the same process and techniques described above during the training process. The set of testing input data and set of testing output data can be the same as or a subset of the training input data and training output data. Alternatively, the set of testing input data and set of testing out data can be different than the training input data and training output data.
  • In [0057] 506, for a profile from the set of profiles used as the testing input data, a diffraction signal is generated using the machine learning system. In 508, the generated diffraction signal is compared with the diffraction signal from the set of diffraction signals in the testing output data that corresponds to the profile. In 510, when the difference between the diffraction signals are not within a desired or predetermined margin of error, the machine learning system is re-trained. When the machine learning system is re-trained, the training process can be adjusted. For example, the selection and number of the training input and output variables can be adjusted. Additionally, the machine learning system can be adjusted. For example, when the machine learning system is a neural network, as described above, the number of hidden nodes can be adjusted. In 512, when the difference between the diffraction signals are within a desired or predetermined margin of error, the testing process is terminated.
  • An empirical risk minimization (ERM) technique can be used to quantify how well the trained machine learning system can generalize to new input. For a more detailed description of ERM, see “Statistical Learning Theory” by Vladimir N. Vapnik, Wiley-Interscience, September 1998, which is incorporated herein by reference in its entirety. [0058]
  • After the machine learning system has been trained and tested, the machine learning system can be used to generate diffraction signals for use in analyzing a structure formed on a semiconductor wafer. Again, it should be noted that the testing process can be omitted in some applications. [0059]
  • With reference to FIG. 6, an [0060] exemplary process 600 is depicted for using a machine learning system to examine a structure formed on a semiconductor wafer. In 602, a measured diffraction signal of the structure is obtained by using a metrology device. In 604, a generated diffraction signal is obtained using the machine learning system. In 606, the diffraction signals are compared. In 608, a feature of the structure is determined based on the comparison of the measured and generated diffraction signals.
  • More particularly, as described above, a profile corresponding to the generated diffraction signal is used as an input to the machine learning system to generate the generated diffraction signal. The profile is characterized by one or more parameters. Thus, when the generated diffraction signal matches the measured diffraction signal within a matching criterion, the profile, and thus the one or more parameters that characterize the profile, can be used to determine a feature of the structure. [0061]
  • With reference to FIG. 7, an [0062] exemplary process 700 is depicted for using a machine learning system in a library-based process. In 702, a library of diffraction signals are generated using the machine learning system. More particularly, the library of diffraction signals is generated by inputting a range of profiles into the machine learning system. In 704, a measured diffraction signal is obtained using a metrology device, such as an ellipsometer, reflectometer, and the like. In 706, the measured diffraction signal is compared to the diffraction signals in the library of diffraction signals generated using the machine learning system. In 708, a feature of the structure is determined using the profile corresponding to the matching diffraction signal from the library of diffraction signals.
  • With reference to FIG. 8, an [0063] exemplary system 800 is depicted for using a machine learning system in a library-based system. As depicted in FIG. 8, library 116 is generated using machine learning system 118. Library 116 is then used by processing module 114 to compare the diffraction signals in library 116 to measured diffraction signals obtained from a metrology device 802, such as an ellipsometer, a reflectometer, and the like. It should be noted that although machine learning system 118 is depicted as a separate unit in FIG. 8, machine learning system 118 can be integrated as a component of processing module 114. Additionally, machine learning system 118 can be connected to processing module 114 to transmit library 116 to processing module 114, such as through a network connection. Alternatively, library 116 can be stored on a portable storage medium and physically transported to processing module 114.
  • Furthermore, as depicted in FIG. 8, [0064] processing module 114 can be coupled to a semiconductor fabrication unit 804 that is configured to perform one or more fabrication steps. It should be recognized, however, that the metrology system can operate as a stand-alone system in addition to being integrated with semiconductor fabrication unit 804.
  • With reference to FIG. 9, an [0065] exemplary process 900 is depicted for using a machine learning system in a regression-based process. In 902, a measured diffraction signal is obtained using a metrology device, such as an ellipsometer, reflectometer, atomic force microscope (AFM), scanning electron microscope (SEM),and the like. In 904, a generated diffraction signal is obtained using the machine learning system. In 906, the two diffraction signals are compared. When the two diffraction signals do not match within a predetermined matching criterion, 904 and 906 are repeated with another diffraction signal generated in 904. This process is iterated until a match is found, meaning that the generated and measured diffraction signals match within the predetermined matching criterion. In 908, if the two diffraction signals match within a predetermined matching criterion, the profile corresponding to the matching diffraction signal is assumed to correspond to the actual profile of the structure being examined. Thus, the profile and the parameters that characterize the profile can be used to determine a feature of the structure.
  • With reference to FIG. 10, an [0066] exemplary system 1000 is depicted for using a machine learning system in a regression-based system. As depicted in FIG. 10, an optimizer 1002 receives the measured diffraction signal as an input from metrology device 802. Optimizer 1002 receives the generated diffraction signal as an input from machine learning system 118. Optimizer 1002 compares the generated and the measured diffraction signals. When the generated and measured diffraction signals do match, optimizer 1002 outputs the profile corresponding to the matching generated diffraction signal. When the generated and measured diffraction signals do not match within a predetermined matching criterion, optimizer 1002 outputs a signal to machine learning system 118 to generate another diffraction signal. This process is iterated until a match is found, meaning that the generated and measured diffraction signals match within the predetermined matching criterion.
  • In one exemplary embodiment, an optimization technique is used to reduce the number of iterations needed to arrive at a match. More particularly, the aim of an optimization problem is to find a best solution among several possible solutions, where the best solution can be quantified by associating a cost function. In other words, for a given problem under a given cost metric, the task is to find a solution with the least cost. Thus, in the present exemplary application, the task is to find the profile with a corresponding diffraction signal that produces the least cost (under a given cost metric) with respect to the given measured diffraction signal. It should be recognized that numerous optimization techniques, which are broadly classified into two categories (i.e., global and local), are known and can be used, such as gradient descent, linear programming, quadratic programming, simulated annealing, Marquardt-Levenberg algorithm, and the like. For a more detailed description of global and local optimization techniques, see “Numerical Recipes in C”, by William H. Press, Saul A. Teukolsky, William T. Vetterling and Brian P. Flannery, Second Edition, Cambridge, which is incorporated herein by reference. [0067]
  • As described above, a library of diffraction signals can be generated as part of a regression-based process. More particularly, when a match has been made, meaning that the generated diffraction signal and the measured diffraction signal match within the matching criterion, a library of diffraction signals can be generated around the matching profile. Generally, the library of diffraction signals generated as part of the regression-based process is smaller than the library that is generated as part of the library-based process described above. [0068]
  • Additionally, the library of diffraction signals generated as part of a regression-based process and the library generated as part of a library-based process described above can be used in an interpolation process, where a solution is derived between two entries in the library. For a more detailed description of an interpolation process, see U.S. patent application Ser. No. 10/075,904, titled PROFILE REFINEMENT FOR INTEGRATED CIRCUIT METROLOGY, filed on Feb. 12, 2002, which is incorporated herein by reference in its entirety. [0069]
  • The foregoing descriptions of specific embodiments of the present invention have been presented for purposes of illustration and description. They are not intended to be exhaustive or to limit the invention to the precise forms disclosed, and it should be understood that many modifications and variations are possible in light of the above teaching. [0070]
  • For example, with reference to FIG. 1, as described above, [0071] machine learning system 118 can be configured to operate with a non-optical metrology device, such as an atomic force microscope (AFM), scanning electron microscopes (SEM), and the like, or a combination of an optical and a non-optical metrology device. Thus, machine learning system 118 can generate various types of diffraction signals corresponding to the type of metrology device used. For example, when the metrology device is a SEM, the diffraction signal generated by machine learning system 118 is a SEM signal, such as two-dimensional images or SEM traces.
  • Additionally, the diffraction signal generated can include characteristic functions of the signal used by the metrology device. For example, during the training process, various order derivatives (e.g., first order, second order . . . n[0072] th order derivatives) of the diffraction signal can be used as part of a Marquardt-Levenberg algorithm to optimize the training process.

Claims (29)

We claim:
1. A method of examining a structure formed on a semiconductor wafer, the method comprising:
obtaining a first diffraction signal measured using an metrology device;
obtaining a second diffraction signal generated using a machine learning system,
wherein the machine learning system receives as an input one or more parameters that characterize a profile of the structure to generate the second diffraction signal;
comparing the first and second diffraction signals; and
when the first and second diffraction signals match within a matching criterion, determining a feature of the structure based on the one or more parameters or the profile used by the machine learning system to generate the second diffraction signal.
2. The method of claim 1, further comprising:
prior to generating the second diffraction signal, training the machine learning system using a set of training input data and a set of training output data,
wherein each of the training input data is a profile of the structure characterized by one or more parameters, and
wherein each of the training output data is a diffraction signal corresponding to the profile of the structure.
3. The method of claim 2, further comprising:
selecting the set of training input data from a range of profiles of the structure.
4. The method of claim 3, further comprising:
dividing the range of profiles into a first partition and at least a second partition,
wherein a first machine learning system is configured and trained for the first partition, and a second machine learning system is configured and trained for the second partition.
5. The method of claim 2, wherein the set of training output data is generated based on the set of training input data using a modeling technique prior to training the machine learning system.
6. The method of claim 5, wherein the modeling technique includes rigorous coupled wave analysis, integral method, Fresnel method, finite analysis, or modal analysis.
7. The method of claim 2, wherein the training output data includes a plurality of dimensions, and further comprising:
transforming the training output data using principal component analysis.
8. The method of claim 7, further comprising:
dividing the dimensions of the training output data into a first partition and at least a second partition,
wherein a first machine learning system is configured and trained for the first partition, and a second machine learning system is configured and trained for the second partition.
9. The method of claim 2, wherein training comprises:
(a) obtaining a training input data;
(b) generating a diffraction signal with the machine learning system using the training input data;
(c) comparing the diffraction signal with the training output data corresponding to the training input data used to generate the diffraction signal;
(d) when the diffraction signal and the training output data do not match within a matching criterion, repeating (b) and (c) with another training input data.
10. The method of claim 2, wherein training comprises using a back-propagation, radial basis network, support vector, or kernel regression algorithm.
11. The method of claim 1, wherein when the first and second diffraction signals do not match within the matching criterion, comparing the first diffraction signal with another diffraction signal from a library of diffraction signals, and wherein the diffraction signals in the library of diffraction signals were generated using the machine learning system.
12. The method of claim 1, wherein when the first and second diffraction signals do not match within the matching criterion, generating another diffraction signal using the machine learning system to compare to the first diffraction signal.
13. The method of claim 1, wherein the metrology device is an ellipsometer, reflectometer, atomic force microscope, or scanning electron microscope.
14. The method of claim 1, wherein the one or more parameters includes one or more of critical dimension measurements, angle of incidence, n and k values, or pitch.
15. The method of claim 1, wherein the machine learning system is a neural network.
16. A computer-readable storage medium containing computer executable instructions for causing a computer to examine a structure formed on a semiconductor wafer, comprising instructions for:
obtaining a first diffraction signal measured using an metrology device;
obtaining a second diffraction signal generated using a machine learning system,
wherein the machine learning system receives as an input one or more parameters that characterize a profile of the structure to generate the second diffraction signal;
comparing the first and second diffraction signals; and
when the first and second diffraction signals match within a matching criterion, determining a feature of the structure based on the one or more parameters of the profile used by the machine learning system to generate the second diffraction signal.
17. The computer-readable storage medium of claim 16, further comprising instructions for:
prior to generating the second diffraction signal, training the machine learning system using a set of training input data and a set of training output data,
wherein each of the training input data is a profile of the structure characterized by one or more parameters, and
wherein each of the training output data is a diffraction signal corresponding to the profile of the structure.
18. The computer-readable storage medium of claim 17, wherein the set of training output data is generated based on the set of training input data using a modeling technique prior to training the machine learning system.
19. The computer-readable storage medium of claim 17, wherein training comprises:
(a) obtaining a training input data;
(b) generating a diffraction signal with the machine learning system using the training input data;
(c) comparing the diffraction signal with the training output data corresponding to the training input data used to generate the diffraction signal;
(d) when the diffraction signal and the training output data do not match within a matching criterion, repeating (b) and (c) with another training input data.
20. The computer-readable storage medium of claim 16, wherein when the first and second diffraction signals do not match within the matching criterion, comparing the first diffraction signal with another diffraction signal from a library of diffraction signals, and wherein the diffraction signals in the library of diffraction signals were generated using the machine learning system.
21. The computer-readable storage medium of claim 16, wherein when the first and second diffraction signals do not match within the matching criterion, generating another diffraction signal using the machine learning system to compare to the first diffraction signal.
22. A system to examine a structure formed on a semiconductor wafer, the system comprising:
an metrology device configured to measure a first diffraction signal from the structure;
a machine learning system configured to generate a second diffraction signal,
wherein the machine learning system receives as an input one or more parameters that characterize a profile of the structure to generate the second diffraction signal; and
a processor configured to compare the first and second diffraction signals,
wherein when the first and second diffraction signals match within a matching criterion, a feature of the structure is determined based on the one or more parameters or the profile used by the machine learning system to generate the second diffraction signal.
23. The system of claim 22, wherein prior to generating the second diffraction signal, the machine learning system is trained using a set of training input data and a set of training output data,
wherein each of the training input data is a profile of the structure characterized by one or more parameters, and
wherein each of the training output data is a diffraction signal corresponding to the profile of the structure.
24. The system of claim 23, wherein the set of training input data is selected from a range of profiles of the structure.
25. The system of claim 24, wherein the range of profiles is divided into a first partition and at least a second partition, and the machine learning system comprises:
a first machine learning system configured and trained for the first partition; and
a second machine learning system configured and trained for the second partition.
26. The system of claim 23, wherein the training output data includes a plurality of dimensions, and the dimensions of the training output data is divided into a first partition and at least a second partition, and wherein the machine learning system comprises:
a first machine learning system configured and trained for the first partition; and
a second machine learning system configured and trained for the second partition.
27. The system of claim 22, further comprising:
a library of diffraction signals, wherein the diffraction signals in the library were generated using the machine learning system,
wherein when the first and second diffraction signals do not match within the matching criterion, the first diffraction signal is compared with another diffraction signal from the library of diffraction signals.
28. The system of claim 22, wherein when the first and second diffraction signals do not match within the matching criterion, the machine learning system generates another diffraction signal to compare to the first diffraction signal.
29. The system of claim 22, further comprising:
a semiconductor fabrication unit coupled to the processor, the semiconductor fabrication unit configured to perform one or more fabrication steps.
US10/608,300 2003-06-27 2003-06-27 Optical metrology of structures formed on semiconductor wafer using machine learning systems Abandoned US20040267397A1 (en)

Priority Applications (7)

Application Number Priority Date Filing Date Title
US10/608,300 US20040267397A1 (en) 2003-06-27 2003-06-27 Optical metrology of structures formed on semiconductor wafer using machine learning systems
PCT/US2004/020682 WO2005003911A2 (en) 2003-06-27 2004-06-25 Optical metrology of structures formed on semiconductor wafers using machine learning systems
KR1020057024949A KR101059427B1 (en) 2003-06-27 2004-06-25 Optical Measurement of Structures Formed on Semiconductor Wafers Using Machine Learning Systems
DE112004001001T DE112004001001T5 (en) 2003-06-27 2004-06-25 Optical measurement of structures formed on semiconductor wafers using machine learning systems
CNB2004800149754A CN100418083C (en) 2003-06-27 2004-06-25 Optical metrology of structures formed on semiconductor wafers using machine learning systems
JP2006517724A JP4589315B2 (en) 2003-06-27 2004-06-25 Optical measurement of structures formed on semiconductor wafers using machine learning systems
US12/399,011 US7831528B2 (en) 2003-06-27 2009-03-05 Optical metrology of structures formed on semiconductor wafers using machine learning systems

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
US10/608,300 US20040267397A1 (en) 2003-06-27 2003-06-27 Optical metrology of structures formed on semiconductor wafer using machine learning systems

Related Child Applications (1)

Application Number Title Priority Date Filing Date
US12/399,011 Continuation US7831528B2 (en) 2003-06-27 2009-03-05 Optical metrology of structures formed on semiconductor wafers using machine learning systems

Publications (1)

Publication Number Publication Date
US20040267397A1 true US20040267397A1 (en) 2004-12-30

Family

ID=33540544

Family Applications (2)

Application Number Title Priority Date Filing Date
US10/608,300 Abandoned US20040267397A1 (en) 2003-06-27 2003-06-27 Optical metrology of structures formed on semiconductor wafer using machine learning systems
US12/399,011 Expired - Fee Related US7831528B2 (en) 2003-06-27 2009-03-05 Optical metrology of structures formed on semiconductor wafers using machine learning systems

Family Applications After (1)

Application Number Title Priority Date Filing Date
US12/399,011 Expired - Fee Related US7831528B2 (en) 2003-06-27 2009-03-05 Optical metrology of structures formed on semiconductor wafers using machine learning systems

Country Status (6)

Country Link
US (2) US20040267397A1 (en)
JP (1) JP4589315B2 (en)
KR (1) KR101059427B1 (en)
CN (1) CN100418083C (en)
DE (1) DE112004001001T5 (en)
WO (1) WO2005003911A2 (en)

Cited By (98)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20040017574A1 (en) * 2002-07-25 2004-01-29 Vi Vuong Model and parameter selection for optical metrology
US20050057748A1 (en) * 2003-09-15 2005-03-17 Timbretechnologies, Inc. Selecting a hypothetical profile to use in optical metrology
US20050088665A1 (en) * 2003-10-28 2005-04-28 Timbre Technologies, Inc. Azimuthal scanning of a structure formed on a semiconductor wafer
US20050192914A1 (en) * 2004-03-01 2005-09-01 Timbre Technologies, Inc. Selecting a profile model for use in optical metrology using a machine learining system
US20050209816A1 (en) * 2004-03-22 2005-09-22 Timbre Technologies, Inc. Optical metrology optimization for repetitive structures
US20050275850A1 (en) * 2004-05-28 2005-12-15 Timbre Technologies, Inc. Shape roughness measurement in optical metrology
US20060046166A1 (en) * 2004-09-01 2006-03-02 Timbre Technologies, Inc. Controlling critical dimensions of structures formed on a wafer in semiconductor processing
US20060064280A1 (en) * 2004-09-21 2006-03-23 Timbre Technologies, Inc. Optical metrology model optimization based on goals
US20060119863A1 (en) * 2004-12-03 2006-06-08 Timbre Technologies, Inc. Examining a structure formed on a semiconductor wafer using machine learning systems
US20060181713A1 (en) * 2005-02-17 2006-08-17 Timbre Technologies, Inc. Optical metrology of a structure formed on a semiconductor wafer using optical pulses
US20060187466A1 (en) * 2005-02-18 2006-08-24 Timbre Technologies, Inc. Selecting unit cell configuration for repeating structures in optical metrology
US20060224528A1 (en) * 2005-03-31 2006-10-05 Timbre Technologies, Inc. Split machine learning systems
US20060290947A1 (en) * 2005-06-16 2006-12-28 Timbre Technologies, Inc. Optical metrology model optimization for repetitive structures
US20070002337A1 (en) * 2005-07-01 2007-01-04 Timbre Technologies, Inc. Modeling and measuring structures with spatially varying properties in optical metrology
US20070211260A1 (en) * 2006-03-08 2007-09-13 Timbre Technologies, Inc. Weighting function to enhance measured diffraction signals in optical metrology
US20070225940A1 (en) * 2006-03-27 2007-09-27 Timbre Technologies Inc. Library accuracy enhancement and evaluation
US20070225851A1 (en) * 2004-07-08 2007-09-27 Timbre Technologies, Inc. Optical metrology model optimization for process control
US20070229806A1 (en) * 2006-03-30 2007-10-04 Tokyo Electron, Ltd. Measuring a damaged structure formed on a wafer using optical metrology
US20070233404A1 (en) * 2006-03-30 2007-10-04 Tokyo Electron, Ltd. Creating a library for measuring a damaged structure formed on a wafer using optical metrology
US20070229854A1 (en) * 2006-03-30 2007-10-04 Timbre Technologies, Inc. Optical metrology of multiple patterned layers
US20070232045A1 (en) * 2006-03-30 2007-10-04 Tokyo Electron, Ltd. Damage assessment of a wafer using optical metrology
US20070229855A1 (en) * 2006-03-30 2007-10-04 Timbre Technologies, Inc. In-die optical metrology
US20070229807A1 (en) * 2006-03-30 2007-10-04 Tokyo Electron, Ltd. Measuring a damaged structure formed on a wafer using optical metrology
US20070250200A1 (en) * 2006-04-21 2007-10-25 Timbre Technologies, Inc. Optimized characterization of wafers structures for optical metrology
US20070268498A1 (en) * 2006-05-22 2007-11-22 Tokyo Electron Limited Matching optical metrology tools using diffraction signals
US20070268497A1 (en) * 2006-05-22 2007-11-22 Tokyo Electron Limited Matching optical metrology tools using hypothetical profiles
US7300730B1 (en) 2006-09-26 2007-11-27 Tokyo Electron Limited Creating an optically tunable anti-reflective coating
US20080009081A1 (en) * 2006-07-10 2008-01-10 Tokyo Electron Limited Managing and using metrology data for process and equipment control
US20080007738A1 (en) * 2006-07-10 2008-01-10 Tokyo Electron Limited Evaluating a profile model to characterize a structure to be examined using optical metrology
US20080007740A1 (en) * 2006-07-10 2008-01-10 Tokyo Electron Limited Optimizing selected variables of an optical metrology model
US20080007739A1 (en) * 2006-07-10 2008-01-10 Tokyo Electron Limited Optimizing selected variables of an optical metrology system
US20080015812A1 (en) * 2006-07-11 2008-01-17 Tokyo Electron Limited Parallel profile determination for an optical metrology system
US20080013107A1 (en) * 2006-07-11 2008-01-17 Tokyo Electron Limited Generating a profile model to characterize a structure to be examined using optical metrology
US20080013108A1 (en) * 2006-07-11 2008-01-17 Tokyo Electron Limited Parallel profile determination in optical metrology
US20080016487A1 (en) * 2006-07-11 2008-01-17 Tokyo Electron Limited Determining position accuracy of double exposure lithography using optical metrology
US20080027565A1 (en) * 2006-07-25 2008-01-31 Tokyo Electron Limited Allocating processing units to generate simulated diffraction signals used in optical metrology
US7327475B1 (en) 2006-12-15 2008-02-05 Tokyo Electron Limited Measuring a process parameter of a semiconductor fabrication process using optical metrology
US20080074678A1 (en) * 2006-09-26 2008-03-27 Tokyo Electron Limited Accuracy of optical metrology measurements
US20080076046A1 (en) * 2006-09-26 2008-03-27 Tokyo Electron Limited accuracy of optical metrology measurements
US20080074677A1 (en) * 2006-09-26 2008-03-27 Tokyo Electron Limited accuracy of optical metrology measurements
US20080077362A1 (en) * 2006-09-26 2008-03-27 Tokyo Electron Limited Methods and apparatus for using an optically tunable soft mask to create a profile library
US20080076045A1 (en) * 2006-09-26 2008-03-27 Tokyo Electron Limited Methods and apparatus for changing the optical properties of resists
US20080089574A1 (en) * 2006-10-12 2008-04-17 Tokyo Electron Limited Data flow management in generating different signal formats used in optical metrology
US20080091724A1 (en) * 2006-10-12 2008-04-17 Tokyo Electron Limited Data flow management in generating profile models used in optical metrology
US20080106729A1 (en) * 2006-11-07 2008-05-08 Tokyo Electron Limited Consecutive measurement of structures formed on a semiconductor wafer using an angle-resolved spectroscopic scatterometer
US20080106728A1 (en) * 2006-11-07 2008-05-08 Tokyo Electron Limited Consecutive measurement of structures formed on a semiconductor wafer using a polarized reflectometer
US7372583B1 (en) 2007-04-12 2008-05-13 Tokyo Electron Limited Controlling a fabrication tool using support vector machine
US20080115140A1 (en) * 2006-09-22 2008-05-15 Tokyo Electron Limited Allocating processing units to processing clusters to generate simulated diffraction signals
US20080117437A1 (en) * 2006-11-16 2008-05-22 Tokyo Electron Limited Drift compensation for an optical metrology tool
US20080144919A1 (en) * 2006-12-14 2008-06-19 Tokyo Electron Limited Determining transmittance of a photomask using optical metrology
US20080170242A1 (en) * 2007-01-12 2008-07-17 Tokyo Electron Limited Determining one or more profile parameters of a structure using optical metrology and a correlation between profile models and key profile shape variables
US20080170241A1 (en) * 2007-01-12 2008-07-17 Tokyo Electron Limited Automated process control using optical metrology and a correlation between profile models and key profile shape variables
US20080231863A1 (en) * 2007-03-20 2008-09-25 Tokyo Electron Limited Automated process control using optical metrology with a photonic nanojet
US20080241975A1 (en) * 2007-03-28 2008-10-02 Tokyo Electron Limited Automated process control using optical metrology and photoresist parameters
US20080243730A1 (en) * 2007-03-28 2008-10-02 Tokyo Electron Limited Training a machine learning system to determine photoresist parameters
US20080255786A1 (en) * 2007-04-12 2008-10-16 Tokyo Electron Limited Optical metrology using support vector machine with profile parameter inputs
US20080255801A1 (en) * 2007-04-12 2008-10-16 Tokyo Electron Limited Optical metrology using a support vector machine with simulated diffraction signal inputs
US20090063077A1 (en) * 2007-08-30 2009-03-05 Tokyo Electron Limited Automated process control using parameters determined with approximation and fine diffraction models
US20090063076A1 (en) * 2007-08-30 2009-03-05 Tokyo Electron Limited Determining profile parameters of a structure using approximation and fine diffraction models in optical metrology
US7505148B2 (en) 2006-11-16 2009-03-17 Tokyo Electron Limited Matching optical metrology tools using spectra enhancement
US20090083013A1 (en) * 2007-09-20 2009-03-26 Tokyo Electron Limited Determining profile parameters of a structure formed on a semiconductor wafer using a dispersion function relating process parameter to dispersion
US20090082993A1 (en) * 2007-09-21 2009-03-26 Tokyo Electron Limited Automated process control of a fabrication tool using a dispersion function relating process parameter to dispersion
US20090116040A1 (en) * 2007-11-07 2009-05-07 Tokyo Electron Limited Method of Deriving an Iso-Dense Bias Using a Hybrid Grating Layer
US20090116010A1 (en) * 2007-11-07 2009-05-07 Tokyo Electron Limited Apparatus for Deriving an Iso-Dense Bias
US20090118857A1 (en) * 2007-11-07 2009-05-07 Tokyo Electron Limited Method of Controlling a Fabrication Process Using an Iso-Dense Bias
US20090248764A1 (en) * 2008-03-27 2009-10-01 Paul R Day Implementing Dynamic Processor Allocation Based Upon Data Density
US20090287637A1 (en) * 2008-05-15 2009-11-19 Day Paul R Determining a Density of a Key Value Referenced in a Database Query Over a Range of Rows
US20090287639A1 (en) * 2008-05-15 2009-11-19 Day Paul R Embedding Densities in a Data Structure
US20090306941A1 (en) * 2006-05-15 2009-12-10 Michael Kotelyanskii Structure Model description and use for scatterometry-based semiconductor manufacturing process metrology
US20100007885A1 (en) * 2008-07-08 2010-01-14 Tokyo Electron Limited Pre-Aligned Metrology System and Modules
US20100007875A1 (en) * 2008-07-08 2010-01-14 Tokyo Electron Limited Field Replaceable Units (FRUs) Optimized for Integrated Metrology (IM)
US20100010765A1 (en) * 2008-07-08 2010-01-14 Tokyo Electron Limited System and Method for Azimuth Angle Calibration
US20100035168A1 (en) * 2008-08-08 2010-02-11 Fumiharu Nakajima Pattern predicting method, recording media and method of fabricating semiconductor device
US20100042388A1 (en) * 2008-08-18 2010-02-18 Joerg Bischoff Computation efficiency by diffraction order truncation
US7728976B2 (en) 2007-03-28 2010-06-01 Tokyo Electron Limited Determining photoresist parameters using optical metrology
US20100145655A1 (en) * 2008-12-09 2010-06-10 Hanyou Chu Rational approximation and continued-fraction approximation approaches for computation efficiency of diffraction signals
US20100201981A1 (en) * 2009-02-12 2010-08-12 Tokyo Electron Limited Calibration method for optical metrology
US20100202055A1 (en) * 2009-02-12 2010-08-12 Tokyo Electron Limited Diffraction order sorting filter for optical metrology
US20100209830A1 (en) * 2009-02-13 2010-08-19 Tokyo Electron Limited Multi-Pitch Scatterometry Targets
US20100214545A1 (en) * 2009-02-24 2010-08-26 Tokyo Electron Limited Creating Metal Gate Structures Using Lithography-Etch-Lithography-Etch (LELE) Processing Sequences
US20110266440A1 (en) * 2010-04-29 2011-11-03 Fei Company SEM Imaging Method
WO2012048156A3 (en) * 2010-10-08 2012-08-02 Tokyo Electron Limited Method of determining an asymmetric property of a structure
US8464194B1 (en) * 2011-12-16 2013-06-11 International Business Machines Corporation Machine learning approach to correct lithographic hot-spots
US20130325395A1 (en) * 2012-06-01 2013-12-05 Globalfoundries Singapore Pte. Ltd. Co-optimization of scatterometry mark design and process monitor mark design
US8745033B2 (en) 2008-01-11 2014-06-03 International Business Machines Corporation Database query optimization using index carryover to subset an index
US8798966B1 (en) * 2007-01-03 2014-08-05 Kla-Tencor Corporation Measuring critical dimensions of a semiconductor structure
EP2791968A4 (en) * 2011-12-16 2015-06-10 Kla Tencor Corp Library generation with derivatives in optical metrology
US20150235108A1 (en) * 2014-02-20 2015-08-20 Kla-Tencor Corporation Signal Response Metrology For Image Based Overlay Measurements
US20150323316A1 (en) * 2014-05-09 2015-11-12 Kla-Tencor Corporation Signal Response Metrology For Scatterometry Based Overlay Measurements
KR20150136524A (en) * 2013-03-27 2015-12-07 케이엘에이-텐코 코포레이션 Statistical model-based metrology
US20160341670A1 (en) * 2015-05-22 2016-11-24 Nanometrics Incorporated Optical metrology using differential fitting
CN107077644A (en) * 2014-11-19 2017-08-18 科磊股份有限公司 System, method and computer program product for combining the initial data from multiple metering outfits
US9977340B2 (en) 2010-06-04 2018-05-22 Asml Netherlands B.V. Method and apparatus for measuring a structure on a substrate, computer program products for implementing such methods and apparatus
DE102018209562B3 (en) 2018-06-14 2019-12-12 Carl Zeiss Smt Gmbh Apparatus and methods for inspecting and / or processing an element for photolithography
WO2020142301A1 (en) * 2019-01-02 2020-07-09 Kla Corporation Machine learning for metrology measurements
US11268805B2 (en) 2019-02-13 2022-03-08 Kioxia Corporation Measurement method
CN114503123A (en) * 2019-10-14 2022-05-13 科磊股份有限公司 Signal domain adaptation for metrology
US11436693B2 (en) 2016-10-12 2022-09-06 Fanuc Corporation Machine learning device and machine learning method for learning correlation between shipment inspection information and operation alarm information for object

Families Citing this family (57)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7634325B2 (en) * 2007-05-03 2009-12-15 Taiwan Semiconductor Manufacturing Company, Ltd. Prediction of uniformity of a wafer
CN101359611B (en) * 2007-07-30 2011-11-09 东京毅力科创株式会社 Selected variable optimization for optical metering system
CN101359612B (en) * 2007-07-30 2012-07-04 东京毅力科创株式会社 Managing and using metering data for process and apparatus control
US7948630B2 (en) * 2008-10-08 2011-05-24 Tokyo Electron Limited Auto focus of a workpiece using two or more focus parameters
KR101467987B1 (en) * 2009-03-02 2014-12-02 어플라이드 머티리얼즈 이스라엘 리미티드 Cd metrology system and method of classifying similar structural elements
MY186210A (en) 2010-07-23 2021-06-30 First Solar Inc In-line metrology system and method
DK3556277T3 (en) 2010-11-30 2021-12-13 Medivators Inc DISPOSABLE SUCTION VALVE FOR AN ENDOSCOPE
CN102207424B (en) * 2010-12-29 2013-01-23 深圳超多维光电子有限公司 Parameter measuring system and method of stereo display device
US8173450B1 (en) 2011-02-14 2012-05-08 Tokyo Electron Limited Method of designing an etch stage measurement system
US8173451B1 (en) 2011-02-16 2012-05-08 Tokyo Electron Limited Etch stage measurement system
US8193007B1 (en) 2011-02-17 2012-06-05 Tokyo Electron Limited Etch process control using optical metrology and sensor devices
US8577820B2 (en) * 2011-03-04 2013-11-05 Tokyo Electron Limited Accurate and fast neural network training for library-based critical dimension (CD) metrology
US8468471B2 (en) 2011-09-23 2013-06-18 Kla-Tencor Corp. Process aware metrology
US10088413B2 (en) * 2011-11-21 2018-10-02 Kla-Tencor Corporation Spectral matching based calibration
US8812277B2 (en) 2011-12-09 2014-08-19 Tokyo Electron Limited Method of enhancing an optical metrology system using ray tracing and flexible ray libraries
US8838422B2 (en) 2011-12-11 2014-09-16 Tokyo Electron Limited Process control using ray tracing-based libraries and machine learning systems
US8570531B2 (en) 2011-12-11 2013-10-29 Tokyo Electron Limited Method of regenerating diffraction signals for optical metrology systems
US10255385B2 (en) 2012-03-28 2019-04-09 Kla-Tencor Corporation Model optimization approach based on spectral sensitivity
US9291554B2 (en) * 2013-02-05 2016-03-22 Kla-Tencor Corporation Method of electromagnetic modeling of finite structures and finite illumination for metrology and inspection
US11175589B2 (en) 2013-06-03 2021-11-16 Kla Corporation Automatic wavelength or angle pruning for optical metrology
US10386729B2 (en) 2013-06-03 2019-08-20 Kla-Tencor Corporation Dynamic removal of correlation of highly correlated parameters for optical metrology
US10481088B2 (en) 2013-06-04 2019-11-19 Kla-Tencor Corporation Automatic determination of fourier harmonic order for computation of spectral information for diffraction structures
US10895810B2 (en) 2013-11-15 2021-01-19 Kla Corporation Automatic selection of sample values for optical metrology
CN104021770B (en) * 2014-06-12 2016-05-11 重庆卓美华视光电有限公司 The processing method of bore hole 3D LCDs module parameter
US10151986B2 (en) * 2014-07-07 2018-12-11 Kla-Tencor Corporation Signal response metrology based on measurements of proxy structures
US9262819B1 (en) 2014-09-26 2016-02-16 GlobalFoundries, Inc. System and method for estimating spatial characteristics of integrated circuits
US10502549B2 (en) * 2015-03-24 2019-12-10 Kla-Tencor Corporation Model-based single parameter measurement
WO2017117568A1 (en) 2015-12-31 2017-07-06 Kla-Tencor Corporation Accelerated training of a machine learning based model for semiconductor applications
US11580375B2 (en) 2015-12-31 2023-02-14 Kla-Tencor Corp. Accelerated training of a machine learning based model for semiconductor applications
US10043261B2 (en) * 2016-01-11 2018-08-07 Kla-Tencor Corp. Generating simulated output for a specimen
US10360477B2 (en) * 2016-01-11 2019-07-23 Kla-Tencor Corp. Accelerating semiconductor-related computations using learning based models
US10921369B2 (en) 2017-01-05 2021-02-16 Xcalipr Corporation High precision optical characterization of carrier transport properties in semiconductors
US10733744B2 (en) * 2017-05-11 2020-08-04 Kla-Tencor Corp. Learning based approach for aligning images acquired with different modalities
WO2019035854A1 (en) * 2017-08-16 2019-02-21 Kla-Tencor Corporation Machine learning in metrology measurements
CN111902924A (en) 2018-03-13 2020-11-06 应用材料公司 Machine learning system for monitoring of semiconductor processing
USD947376S1 (en) 2018-03-21 2022-03-29 Medivators Inc. Endoscope suction valve
KR20200130870A (en) * 2018-04-10 2020-11-20 램 리써치 코포레이션 Optical instrumentation in machine learning to characterize features
US20230045798A1 (en) * 2018-04-30 2023-02-16 Seoul National University R&Db Foundation Method for predicting structure of indoor space using radio propagation channel analysis through deep learning
USD952142S1 (en) 2018-05-21 2022-05-17 Medivators Inc. Cleaning adapter
JP6974635B2 (en) 2018-06-14 2021-12-01 ノヴァ リミテッドNova Ltd Semiconductor manufacturing measurement and processing control
EP3629088A1 (en) * 2018-09-28 2020-04-01 ASML Netherlands B.V. Providing a trained neural network and determining a characteristic of a physical system
US10705514B2 (en) * 2018-10-09 2020-07-07 Applied Materials, Inc. Adaptive chamber matching in advanced semiconductor process control
US10657214B2 (en) 2018-10-09 2020-05-19 Applied Materials, Inc. Predictive spatial digital design of experiment for advanced semiconductor process optimization and control
US10930531B2 (en) 2018-10-09 2021-02-23 Applied Materials, Inc. Adaptive control of wafer-to-wafer variability in device performance in advanced semiconductor processes
KR102224466B1 (en) 2018-11-07 2021-03-05 포항공과대학교 산학협력단 An analyzing method for perovskite structure using machine learning
DE102019103503A1 (en) * 2019-02-12 2020-08-13 Carl Zeiss Smt Gmbh Error reduction in images that were generated with charged particles using machine learning-based methods
JP7316867B2 (en) 2019-07-25 2023-07-28 キオクシア株式会社 Semiconductor image processing device
KR102230354B1 (en) * 2019-11-18 2021-03-22 고려대학교 산학협력단 Apparatus and method of testing semiconductor device by using machine learning model
CN111043988B (en) * 2019-12-10 2021-04-23 东南大学 Single stripe projection measurement method based on graphics and deep learning
US11092901B2 (en) * 2019-12-21 2021-08-17 Qoniac Gmbh Wafer exposure method using wafer models and wafer fabrication assembly
JP6832463B1 (en) * 2020-04-06 2021-02-24 東京応化工業株式会社 Information processing system, information processing device, information processing method and program
CN111595812B (en) * 2020-05-29 2021-06-22 复旦大学 Method and system for measuring key parameters based on momentum space dispersion relation
US11289387B2 (en) 2020-07-31 2022-03-29 Applied Materials, Inc. Methods and apparatus for backside via reveal processing
KR102468352B1 (en) * 2021-02-26 2022-11-18 김이경 Structure designing method for controlling wave distribution and apparatus therefor
US20220375051A1 (en) * 2021-05-05 2022-11-24 Kla Corporation Deep generative model-based alignment for semiconductor applications
US20220388112A1 (en) * 2021-06-03 2022-12-08 Applied Materials, Inc. Using light coupling properties for machine-learning-based film detection
US20240062097A1 (en) * 2022-08-22 2024-02-22 Applied Materials, Inc. Equipment parameter management at a manufacturing system using machine learning

Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5479573A (en) * 1992-11-24 1995-12-26 Pavilion Technologies, Inc. Predictive network with learned preprocessing parameters
US5793480A (en) * 1995-09-01 1998-08-11 Phase Metrics, Inc. Combined interferometer/ellipsometer for measuring small spacings
US6192103B1 (en) * 1999-06-03 2001-02-20 Bede Scientific, Inc. Fitting of X-ray scattering data using evolutionary algorithms
US6650422B2 (en) * 2001-03-26 2003-11-18 Advanced Micro Devices, Inc. Scatterometry techniques to ascertain asymmetry profile of features and generate a feedback or feedforward process control data associated therewith
US6657736B1 (en) * 1999-07-09 2003-12-02 Nova Measuring Instruments Ltd. Method and system for measuring patterned structures
US6665446B1 (en) * 1998-12-25 2003-12-16 Canon Kabushiki Kaisha Image processing apparatus and method

Family Cites Families (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2001185595A (en) * 1999-12-27 2001-07-06 Fujitsu Ltd Method for controlling characteristic parameters
US6943900B2 (en) * 2000-09-15 2005-09-13 Timbre Technologies, Inc. Generation of a library of periodic grating diffraction signals
US6558965B1 (en) * 2001-07-11 2003-05-06 Advanced Micro Devices, Inc. Measuring BARC thickness using scatterometry
US6785638B2 (en) * 2001-08-06 2004-08-31 Timbre Technologies, Inc. Method and system of dynamic learning through a regression-based library generation process
US7031894B2 (en) * 2002-01-16 2006-04-18 Timbre Technologies, Inc. Generating a library of simulated-diffraction signals and hypothetical profiles of periodic gratings

Patent Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5479573A (en) * 1992-11-24 1995-12-26 Pavilion Technologies, Inc. Predictive network with learned preprocessing parameters
US5793480A (en) * 1995-09-01 1998-08-11 Phase Metrics, Inc. Combined interferometer/ellipsometer for measuring small spacings
US6665446B1 (en) * 1998-12-25 2003-12-16 Canon Kabushiki Kaisha Image processing apparatus and method
US6192103B1 (en) * 1999-06-03 2001-02-20 Bede Scientific, Inc. Fitting of X-ray scattering data using evolutionary algorithms
US6657736B1 (en) * 1999-07-09 2003-12-02 Nova Measuring Instruments Ltd. Method and system for measuring patterned structures
US6650422B2 (en) * 2001-03-26 2003-11-18 Advanced Micro Devices, Inc. Scatterometry techniques to ascertain asymmetry profile of features and generate a feedback or feedforward process control data associated therewith

Cited By (200)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20080151269A1 (en) * 2002-07-25 2008-06-26 Timbre Technologies, Inc. Model and parameter selection for optical metrology
US7505153B2 (en) 2002-07-25 2009-03-17 Timbre Technologies, Inc. Model and parameter selection for optical metrology
US7330279B2 (en) 2002-07-25 2008-02-12 Timbre Technologies, Inc. Model and parameter selection for optical metrology
US20040017574A1 (en) * 2002-07-25 2004-01-29 Vi Vuong Model and parameter selection for optical metrology
US7394554B2 (en) 2003-09-15 2008-07-01 Timbre Technologies, Inc. Selecting a hypothetical profile to use in optical metrology
US20050057748A1 (en) * 2003-09-15 2005-03-17 Timbretechnologies, Inc. Selecting a hypothetical profile to use in optical metrology
US20050088665A1 (en) * 2003-10-28 2005-04-28 Timbre Technologies, Inc. Azimuthal scanning of a structure formed on a semiconductor wafer
US7414733B2 (en) 2003-10-28 2008-08-19 Timbre Technologies, Inc. Azimuthal scanning of a structure formed on a semiconductor wafer
US20070236705A1 (en) * 2003-10-28 2007-10-11 Timbre Technologies Inc. Azimuthal scanning of a structure formed on a semiconductor wafer
US7224471B2 (en) 2003-10-28 2007-05-29 Timbre Technologies, Inc. Azimuthal scanning of a structure formed on a semiconductor wafer
US20050192914A1 (en) * 2004-03-01 2005-09-01 Timbre Technologies, Inc. Selecting a profile model for use in optical metrology using a machine learining system
US7523076B2 (en) * 2004-03-01 2009-04-21 Tokyo Electron Limited Selecting a profile model for use in optical metrology using a machine learning system
US20050209816A1 (en) * 2004-03-22 2005-09-22 Timbre Technologies, Inc. Optical metrology optimization for repetitive structures
US7388677B2 (en) 2004-03-22 2008-06-17 Timbre Technologies, Inc. Optical metrology optimization for repetitive structures
US20050275850A1 (en) * 2004-05-28 2005-12-15 Timbre Technologies, Inc. Shape roughness measurement in optical metrology
US20070225851A1 (en) * 2004-07-08 2007-09-27 Timbre Technologies, Inc. Optical metrology model optimization for process control
US7395132B2 (en) * 2004-07-08 2008-07-01 Timbre Technologies, Inc. Optical metrology model optimization for process control
US20060046166A1 (en) * 2004-09-01 2006-03-02 Timbre Technologies, Inc. Controlling critical dimensions of structures formed on a wafer in semiconductor processing
US7566181B2 (en) 2004-09-01 2009-07-28 Tokyo Electron Limited Controlling critical dimensions of structures formed on a wafer in semiconductor processing
US7588949B2 (en) 2004-09-21 2009-09-15 Tokyo Electron Limited Optical metrology model optimization based on goals
US7171284B2 (en) 2004-09-21 2007-01-30 Timbre Technologies, Inc. Optical metrology model optimization based on goals
US20060064280A1 (en) * 2004-09-21 2006-03-23 Timbre Technologies, Inc. Optical metrology model optimization based on goals
US20060119863A1 (en) * 2004-12-03 2006-06-08 Timbre Technologies, Inc. Examining a structure formed on a semiconductor wafer using machine learning systems
US7453584B2 (en) 2004-12-03 2008-11-18 Timbre Technologies, Inc. Examining a structure formed on a semiconductor wafer using machine learning systems
US20080033683A1 (en) * 2004-12-03 2008-02-07 Timbre Technologies, Inc. Examining a structure formed on a semiconductor wafer using machine learning systems
US7280229B2 (en) 2004-12-03 2007-10-09 Timbre Technologies, Inc. Examining a structure formed on a semiconductor wafer using machine learning systems
US7274465B2 (en) * 2005-02-17 2007-09-25 Timbre Technologies, Inc. Optical metrology of a structure formed on a semiconductor wafer using optical pulses
US20060181713A1 (en) * 2005-02-17 2006-08-17 Timbre Technologies, Inc. Optical metrology of a structure formed on a semiconductor wafer using optical pulses
US7616325B2 (en) 2005-02-18 2009-11-10 Tokyo Electron Limited Optical metrology optimization for repetitive structures
US20060187466A1 (en) * 2005-02-18 2006-08-24 Timbre Technologies, Inc. Selecting unit cell configuration for repeating structures in optical metrology
US20080285054A1 (en) * 2005-02-18 2008-11-20 Timbre Technologies, Inc. Optical metrology optimization for repetitive structures
US20060224528A1 (en) * 2005-03-31 2006-10-05 Timbre Technologies, Inc. Split machine learning systems
US7421414B2 (en) * 2005-03-31 2008-09-02 Timbre Technologies, Inc. Split machine learning systems
US20060290947A1 (en) * 2005-06-16 2006-12-28 Timbre Technologies, Inc. Optical metrology model optimization for repetitive structures
US7355728B2 (en) 2005-06-16 2008-04-08 Timbre Technologies, Inc. Optical metrology model optimization for repetitive structures
US20080195342A1 (en) * 2005-06-16 2008-08-14 Timbre Technologies, Inc. Optical metrology model optimization for repetitive structures
US20070002337A1 (en) * 2005-07-01 2007-01-04 Timbre Technologies, Inc. Modeling and measuring structures with spatially varying properties in optical metrology
US7515282B2 (en) 2005-07-01 2009-04-07 Timbre Technologies, Inc. Modeling and measuring structures with spatially varying properties in optical metrology
US20070211260A1 (en) * 2006-03-08 2007-09-13 Timbre Technologies, Inc. Weighting function to enhance measured diffraction signals in optical metrology
US7523021B2 (en) 2006-03-08 2009-04-21 Tokyo Electron Limited Weighting function to enhance measured diffraction signals in optical metrology
US7617075B2 (en) 2006-03-27 2009-11-10 Tokyo Electron Limited Library accuracy enhancment and evaluation
US7302367B2 (en) 2006-03-27 2007-11-27 Timbre Technologies, Inc. Library accuracy enhancement and evaluation
US20080071504A1 (en) * 2006-03-27 2008-03-20 Timbre Technologies Inc. Library accuracy enhancment and evaluation
US20070225940A1 (en) * 2006-03-27 2007-09-27 Timbre Technologies Inc. Library accuracy enhancement and evaluation
US20070233404A1 (en) * 2006-03-30 2007-10-04 Tokyo Electron, Ltd. Creating a library for measuring a damaged structure formed on a wafer using optical metrology
US20070229807A1 (en) * 2006-03-30 2007-10-04 Tokyo Electron, Ltd. Measuring a damaged structure formed on a wafer using optical metrology
US7522293B2 (en) 2006-03-30 2009-04-21 Tokyo Electron Limited Optical metrology of multiple patterned layers
US7324193B2 (en) * 2006-03-30 2008-01-29 Tokyo Electron Limited Measuring a damaged structure formed on a wafer using optical metrology
US20080137078A1 (en) * 2006-03-30 2008-06-12 Tokyo Electron Limited Measuring a damaged structure formed on a wafer using optical metrology
US7623978B2 (en) 2006-03-30 2009-11-24 Tokyo Electron Limited Damage assessment of a wafer using optical metrology
US20070229855A1 (en) * 2006-03-30 2007-10-04 Timbre Technologies, Inc. In-die optical metrology
US7619731B2 (en) 2006-03-30 2009-11-17 Tokyo Electron Limited Measuring a damaged structure formed on a wafer using optical metrology
US20070232045A1 (en) * 2006-03-30 2007-10-04 Tokyo Electron, Ltd. Damage assessment of a wafer using optical metrology
US20070229854A1 (en) * 2006-03-30 2007-10-04 Timbre Technologies, Inc. Optical metrology of multiple patterned layers
US20070229806A1 (en) * 2006-03-30 2007-10-04 Tokyo Electron, Ltd. Measuring a damaged structure formed on a wafer using optical metrology
US7474420B2 (en) 2006-03-30 2009-01-06 Timbre Technologies, Inc. In-die optical metrology
US7576851B2 (en) 2006-03-30 2009-08-18 Tokyo Electron Limited Creating a library for measuring a damaged structure formed on a wafer using optical metrology
US7444196B2 (en) * 2006-04-21 2008-10-28 Timbre Technologies, Inc. Optimized characterization of wafers structures for optical metrology
US20070250200A1 (en) * 2006-04-21 2007-10-25 Timbre Technologies, Inc. Optimized characterization of wafers structures for optical metrology
WO2007124155A2 (en) * 2006-04-21 2007-11-01 Tokyo Electron Limited Optimized characterization of wafer structures for optical metrology
WO2007124155A3 (en) * 2006-04-21 2008-11-13 Tokyo Electron Ltd Optimized characterization of wafer structures for optical metrology
US20090306941A1 (en) * 2006-05-15 2009-12-10 Michael Kotelyanskii Structure Model description and use for scatterometry-based semiconductor manufacturing process metrology
US7446888B2 (en) 2006-05-22 2008-11-04 Tokyo Electron Limited Matching optical metrology tools using diffraction signals
US7446887B2 (en) 2006-05-22 2008-11-04 Tokyo Electron Limited Matching optical metrology tools using hypothetical profiles
US20070268498A1 (en) * 2006-05-22 2007-11-22 Tokyo Electron Limited Matching optical metrology tools using diffraction signals
US20070268497A1 (en) * 2006-05-22 2007-11-22 Tokyo Electron Limited Matching optical metrology tools using hypothetical profiles
US20080007739A1 (en) * 2006-07-10 2008-01-10 Tokyo Electron Limited Optimizing selected variables of an optical metrology system
US7526354B2 (en) 2006-07-10 2009-04-28 Tokyo Electron Limited Managing and using metrology data for process and equipment control
US7495781B2 (en) 2006-07-10 2009-02-24 Tokyo Electron Limited Optimizing selected variables of an optical metrology model
US20080009081A1 (en) * 2006-07-10 2008-01-10 Tokyo Electron Limited Managing and using metrology data for process and equipment control
US20080007738A1 (en) * 2006-07-10 2008-01-10 Tokyo Electron Limited Evaluating a profile model to characterize a structure to be examined using optical metrology
US7525673B2 (en) 2006-07-10 2009-04-28 Tokyo Electron Limited Optimizing selected variables of an optical metrology system
US20080007740A1 (en) * 2006-07-10 2008-01-10 Tokyo Electron Limited Optimizing selected variables of an optical metrology model
US7518740B2 (en) 2006-07-10 2009-04-14 Tokyo Electron Limited Evaluating a profile model to characterize a structure to be examined using optical metrology
US7515283B2 (en) 2006-07-11 2009-04-07 Tokyo Electron, Ltd. Parallel profile determination in optical metrology
US7523439B2 (en) 2006-07-11 2009-04-21 Tokyo Electron Limited Determining position accuracy of double exposure lithography using optical metrology
US7469192B2 (en) 2006-07-11 2008-12-23 Tokyo Electron Ltd. Parallel profile determination for an optical metrology system
US20080015812A1 (en) * 2006-07-11 2008-01-17 Tokyo Electron Limited Parallel profile determination for an optical metrology system
US20080013107A1 (en) * 2006-07-11 2008-01-17 Tokyo Electron Limited Generating a profile model to characterize a structure to be examined using optical metrology
US20080013108A1 (en) * 2006-07-11 2008-01-17 Tokyo Electron Limited Parallel profile determination in optical metrology
US20080016487A1 (en) * 2006-07-11 2008-01-17 Tokyo Electron Limited Determining position accuracy of double exposure lithography using optical metrology
US7742888B2 (en) 2006-07-25 2010-06-22 Tokyo Electron Limited Allocating processing units to generate simulated diffraction signals used in optical metrology
US20080027565A1 (en) * 2006-07-25 2008-01-31 Tokyo Electron Limited Allocating processing units to generate simulated diffraction signals used in optical metrology
US20080115140A1 (en) * 2006-09-22 2008-05-15 Tokyo Electron Limited Allocating processing units to processing clusters to generate simulated diffraction signals
US7765076B2 (en) 2006-09-22 2010-07-27 Tokyo Electron Limited Allocating processing units to processing clusters to generate simulated diffraction signals
US20080074677A1 (en) * 2006-09-26 2008-03-27 Tokyo Electron Limited accuracy of optical metrology measurements
US20080074678A1 (en) * 2006-09-26 2008-03-27 Tokyo Electron Limited Accuracy of optical metrology measurements
US20080076046A1 (en) * 2006-09-26 2008-03-27 Tokyo Electron Limited accuracy of optical metrology measurements
US7300730B1 (en) 2006-09-26 2007-11-27 Tokyo Electron Limited Creating an optically tunable anti-reflective coating
US7763404B2 (en) 2006-09-26 2010-07-27 Tokyo Electron Limited Methods and apparatus for changing the optical properties of resists
US7555395B2 (en) 2006-09-26 2009-06-30 Tokyo Electron Limited Methods and apparatus for using an optically tunable soft mask to create a profile library
US20080077362A1 (en) * 2006-09-26 2008-03-27 Tokyo Electron Limited Methods and apparatus for using an optically tunable soft mask to create a profile library
US20080076045A1 (en) * 2006-09-26 2008-03-27 Tokyo Electron Limited Methods and apparatus for changing the optical properties of resists
US7783669B2 (en) 2006-10-12 2010-08-24 Tokyo Electron Limited Data flow management in generating profile models used in optical metrology
US7765234B2 (en) 2006-10-12 2010-07-27 Tokyo Electron Limited Data flow management in generating different signal formats used in optical metrology
US20080091724A1 (en) * 2006-10-12 2008-04-17 Tokyo Electron Limited Data flow management in generating profile models used in optical metrology
US20080089574A1 (en) * 2006-10-12 2008-04-17 Tokyo Electron Limited Data flow management in generating different signal formats used in optical metrology
US7417750B2 (en) 2006-11-07 2008-08-26 Tokyo Electron Limited Consecutive measurement of structures formed on a semiconductor wafer using an angle-resolved spectroscopic scatterometer
US20080106729A1 (en) * 2006-11-07 2008-05-08 Tokyo Electron Limited Consecutive measurement of structures formed on a semiconductor wafer using an angle-resolved spectroscopic scatterometer
US7522295B2 (en) 2006-11-07 2009-04-21 Tokyo Electron Limited Consecutive measurement of structures formed on a semiconductor wafer using a polarized reflectometer
US20080106728A1 (en) * 2006-11-07 2008-05-08 Tokyo Electron Limited Consecutive measurement of structures formed on a semiconductor wafer using a polarized reflectometer
US7428044B2 (en) 2006-11-16 2008-09-23 Tokyo Electron Limited Drift compensation for an optical metrology tool
US7505148B2 (en) 2006-11-16 2009-03-17 Tokyo Electron Limited Matching optical metrology tools using spectra enhancement
US20080117437A1 (en) * 2006-11-16 2008-05-22 Tokyo Electron Limited Drift compensation for an optical metrology tool
US7639375B2 (en) 2006-12-14 2009-12-29 Tokyo Electron Limited Determining transmittance of a photomask using optical metrology
US20080144919A1 (en) * 2006-12-14 2008-06-19 Tokyo Electron Limited Determining transmittance of a photomask using optical metrology
US20080212080A1 (en) * 2006-12-15 2008-09-04 Tokyo Electron Limited Measuring a process parameter of a semiconductor fabrication process using optical metrology
US7522294B2 (en) 2006-12-15 2009-04-21 Tokyo Electron Limited Measuring a process parameter of a semiconductor fabrication process using optical metrology
US7327475B1 (en) 2006-12-15 2008-02-05 Tokyo Electron Limited Measuring a process parameter of a semiconductor fabrication process using optical metrology
US8798966B1 (en) * 2007-01-03 2014-08-05 Kla-Tencor Corporation Measuring critical dimensions of a semiconductor structure
US20080170242A1 (en) * 2007-01-12 2008-07-17 Tokyo Electron Limited Determining one or more profile parameters of a structure using optical metrology and a correlation between profile models and key profile shape variables
US20080170241A1 (en) * 2007-01-12 2008-07-17 Tokyo Electron Limited Automated process control using optical metrology and a correlation between profile models and key profile shape variables
US7667858B2 (en) 2007-01-12 2010-02-23 Tokyo Electron Limited Automated process control using optical metrology and a correlation between profile models and key profile shape variables
US7596422B2 (en) 2007-01-12 2009-09-29 Tokyo Electron Limited Determining one or more profile parameters of a structure using optical metrology and a correlation between profile models and key profile shape variables
US20080231863A1 (en) * 2007-03-20 2008-09-25 Tokyo Electron Limited Automated process control using optical metrology with a photonic nanojet
US7639351B2 (en) 2007-03-20 2009-12-29 Tokyo Electron Limited Automated process control using optical metrology with a photonic nanojet
US7567353B2 (en) 2007-03-28 2009-07-28 Tokyo Electron Limited Automated process control using optical metrology and photoresist parameters
US20080241975A1 (en) * 2007-03-28 2008-10-02 Tokyo Electron Limited Automated process control using optical metrology and photoresist parameters
US7949618B2 (en) 2007-03-28 2011-05-24 Tokyo Electron Limited Training a machine learning system to determine photoresist parameters
US20080243730A1 (en) * 2007-03-28 2008-10-02 Tokyo Electron Limited Training a machine learning system to determine photoresist parameters
US7728976B2 (en) 2007-03-28 2010-06-01 Tokyo Electron Limited Determining photoresist parameters using optical metrology
US7372583B1 (en) 2007-04-12 2008-05-13 Tokyo Electron Limited Controlling a fabrication tool using support vector machine
US7567352B2 (en) 2007-04-12 2009-07-28 Tokyo Electron Limited Controlling a fabrication tool using support vector machine
US20080252908A1 (en) * 2007-04-12 2008-10-16 Tokyo Electron Limited Controlling a fabrication tool using support vector machine
US20080255786A1 (en) * 2007-04-12 2008-10-16 Tokyo Electron Limited Optical metrology using support vector machine with profile parameter inputs
US7511835B2 (en) 2007-04-12 2009-03-31 Tokyo Electron Limited Optical metrology using a support vector machine with simulated diffraction signal inputs
US20080255801A1 (en) * 2007-04-12 2008-10-16 Tokyo Electron Limited Optical metrology using a support vector machine with simulated diffraction signal inputs
US7483809B2 (en) 2007-04-12 2009-01-27 Tokyo Electron Limited Optical metrology using support vector machine with profile parameter inputs
US20090063077A1 (en) * 2007-08-30 2009-03-05 Tokyo Electron Limited Automated process control using parameters determined with approximation and fine diffraction models
US7949490B2 (en) 2007-08-30 2011-05-24 Tokyo Electron Limited Determining profile parameters of a structure using approximation and fine diffraction models in optical metrology
US7627392B2 (en) 2007-08-30 2009-12-01 Tokyo Electron Limited Automated process control using parameters determined with approximation and fine diffraction models
US20090063076A1 (en) * 2007-08-30 2009-03-05 Tokyo Electron Limited Determining profile parameters of a structure using approximation and fine diffraction models in optical metrology
US7912679B2 (en) * 2007-09-20 2011-03-22 Tokyo Electron Limited Determining profile parameters of a structure formed on a semiconductor wafer using a dispersion function relating process parameter to dispersion
US20090083013A1 (en) * 2007-09-20 2009-03-26 Tokyo Electron Limited Determining profile parameters of a structure formed on a semiconductor wafer using a dispersion function relating process parameter to dispersion
US20090082993A1 (en) * 2007-09-21 2009-03-26 Tokyo Electron Limited Automated process control of a fabrication tool using a dispersion function relating process parameter to dispersion
US7636649B2 (en) * 2007-09-21 2009-12-22 Tokyo Electron Limited Automated process control of a fabrication tool using a dispersion function relating process parameter to dispersion
US20090118857A1 (en) * 2007-11-07 2009-05-07 Tokyo Electron Limited Method of Controlling a Fabrication Process Using an Iso-Dense Bias
US7639370B2 (en) 2007-11-07 2009-12-29 Tokyo Electron Limited Apparatus for deriving an iso-dense bias
US20090116010A1 (en) * 2007-11-07 2009-05-07 Tokyo Electron Limited Apparatus for Deriving an Iso-Dense Bias
US7598099B2 (en) 2007-11-07 2009-10-06 Tokyo Electron Limited Method of controlling a fabrication process using an iso-dense bias
US20090116040A1 (en) * 2007-11-07 2009-05-07 Tokyo Electron Limited Method of Deriving an Iso-Dense Bias Using a Hybrid Grating Layer
US8745033B2 (en) 2008-01-11 2014-06-03 International Business Machines Corporation Database query optimization using index carryover to subset an index
US8015191B2 (en) * 2008-03-27 2011-09-06 International Business Machines Corporation Implementing dynamic processor allocation based upon data density
US20090248764A1 (en) * 2008-03-27 2009-10-01 Paul R Day Implementing Dynamic Processor Allocation Based Upon Data Density
US20090287637A1 (en) * 2008-05-15 2009-11-19 Day Paul R Determining a Density of a Key Value Referenced in a Database Query Over a Range of Rows
US10387411B2 (en) 2008-05-15 2019-08-20 International Business Machines Corporation Determining a density of a key value referenced in a database query over a range of rows
US8140520B2 (en) 2008-05-15 2012-03-20 International Business Machines Corporation Embedding densities in a data structure
US8396861B2 (en) 2008-05-15 2013-03-12 International Business Machines Corporation Determining a density of a key value referenced in a database query over a range of rows
US8275761B2 (en) 2008-05-15 2012-09-25 International Business Machines Corporation Determining a density of a key value referenced in a database query over a range of rows
US20090287639A1 (en) * 2008-05-15 2009-11-19 Day Paul R Embedding Densities in a Data Structure
US20100007875A1 (en) * 2008-07-08 2010-01-14 Tokyo Electron Limited Field Replaceable Units (FRUs) Optimized for Integrated Metrology (IM)
US7990534B2 (en) 2008-07-08 2011-08-02 Tokyo Electron Limited System and method for azimuth angle calibration
US20100007885A1 (en) * 2008-07-08 2010-01-14 Tokyo Electron Limited Pre-Aligned Metrology System and Modules
US7940391B2 (en) 2008-07-08 2011-05-10 Tokyo Electron Limited Pre-aligned metrology system and modules
US7742163B2 (en) 2008-07-08 2010-06-22 Tokyo Electron Limited Field replaceable units (FRUs) optimized for integrated metrology (IM)
US20100010765A1 (en) * 2008-07-08 2010-01-14 Tokyo Electron Limited System and Method for Azimuth Angle Calibration
US20100035168A1 (en) * 2008-08-08 2010-02-11 Fumiharu Nakajima Pattern predicting method, recording media and method of fabricating semiconductor device
US20100042388A1 (en) * 2008-08-18 2010-02-18 Joerg Bischoff Computation efficiency by diffraction order truncation
US9625937B2 (en) 2008-08-18 2017-04-18 Kla-Tencor Corporation Computation efficiency by diffraction order truncation
US20100145655A1 (en) * 2008-12-09 2010-06-10 Hanyou Chu Rational approximation and continued-fraction approximation approaches for computation efficiency of diffraction signals
US8560270B2 (en) * 2008-12-09 2013-10-15 Tokyo Electron Limited Rational approximation and continued-fraction approximation approaches for computation efficiency of diffraction signals
US20100202055A1 (en) * 2009-02-12 2010-08-12 Tokyo Electron Limited Diffraction order sorting filter for optical metrology
US7924422B2 (en) 2009-02-12 2011-04-12 Tokyo Electron Limited Calibration method for optical metrology
US8107073B2 (en) 2009-02-12 2012-01-31 Tokyo Electron Limited Diffraction order sorting filter for optical metrology
US20100201981A1 (en) * 2009-02-12 2010-08-12 Tokyo Electron Limited Calibration method for optical metrology
US20100209830A1 (en) * 2009-02-13 2010-08-19 Tokyo Electron Limited Multi-Pitch Scatterometry Targets
US8024676B2 (en) 2009-02-13 2011-09-20 Tokyo Electron Limited Multi-pitch scatterometry targets
US8183062B2 (en) 2009-02-24 2012-05-22 Tokyo Electron Limited Creating metal gate structures using Lithography-Etch-Lithography-Etch (LELE) processing sequences
US20100214545A1 (en) * 2009-02-24 2010-08-26 Tokyo Electron Limited Creating Metal Gate Structures Using Lithography-Etch-Lithography-Etch (LELE) Processing Sequences
US8232523B2 (en) * 2010-04-29 2012-07-31 Fei Company SEM imaging method
US20110266440A1 (en) * 2010-04-29 2011-11-03 Fei Company SEM Imaging Method
US9977340B2 (en) 2010-06-04 2018-05-22 Asml Netherlands B.V. Method and apparatus for measuring a structure on a substrate, computer program products for implementing such methods and apparatus
US9239522B2 (en) 2010-10-08 2016-01-19 Kla-Tencor Corporation Method of determining an asymmetric property of a structure
WO2012048156A3 (en) * 2010-10-08 2012-08-02 Tokyo Electron Limited Method of determining an asymmetric property of a structure
US8464194B1 (en) * 2011-12-16 2013-06-11 International Business Machines Corporation Machine learning approach to correct lithographic hot-spots
EP2791968A4 (en) * 2011-12-16 2015-06-10 Kla Tencor Corp Library generation with derivatives in optical metrology
US20130325395A1 (en) * 2012-06-01 2013-12-05 Globalfoundries Singapore Pte. Ltd. Co-optimization of scatterometry mark design and process monitor mark design
KR20150136524A (en) * 2013-03-27 2015-12-07 케이엘에이-텐코 코포레이션 Statistical model-based metrology
US10101670B2 (en) 2013-03-27 2018-10-16 Kla-Tencor Corporation Statistical model-based metrology
KR102035376B1 (en) 2013-03-27 2019-10-23 케이엘에이 코포레이션 Statistical model-based metrology
EP2979297A4 (en) * 2013-03-27 2017-02-22 Kla-Tencor Corporation Statistical model-based metrology
KR20160124775A (en) * 2014-02-20 2016-10-28 케이엘에이-텐코 코포레이션 Signal response metrology for image based overlay measurements
US10152654B2 (en) * 2014-02-20 2018-12-11 Kla-Tencor Corporation Signal response metrology for image based overlay measurements
US20150235108A1 (en) * 2014-02-20 2015-08-20 Kla-Tencor Corporation Signal Response Metrology For Image Based Overlay Measurements
KR102184029B1 (en) 2014-02-20 2020-11-27 케이엘에이 코포레이션 Signal response metrology for image based overlay measurements
KR102221063B1 (en) 2014-05-09 2021-02-25 케이엘에이 코포레이션 Signal response metrology for scatterometry based overlay measurements
KR20170005059A (en) * 2014-05-09 2017-01-11 케이엘에이-텐코 코포레이션 Signal response metrology for scatterometry based overlay measurements
US10352876B2 (en) * 2014-05-09 2019-07-16 KLA—Tencor Corporation Signal response metrology for scatterometry based overlay measurements
US20150323316A1 (en) * 2014-05-09 2015-11-12 Kla-Tencor Corporation Signal Response Metrology For Scatterometry Based Overlay Measurements
CN107077644A (en) * 2014-11-19 2017-08-18 科磊股份有限公司 System, method and computer program product for combining the initial data from multiple metering outfits
US9995689B2 (en) * 2015-05-22 2018-06-12 Nanometrics Incorporated Optical metrology using differential fitting
US20160341670A1 (en) * 2015-05-22 2016-11-24 Nanometrics Incorporated Optical metrology using differential fitting
US11436693B2 (en) 2016-10-12 2022-09-06 Fanuc Corporation Machine learning device and machine learning method for learning correlation between shipment inspection information and operation alarm information for object
DE102018209562B3 (en) 2018-06-14 2019-12-12 Carl Zeiss Smt Gmbh Apparatus and methods for inspecting and / or processing an element for photolithography
US11410290B2 (en) 2019-01-02 2022-08-09 Kla Corporation Machine learning for metrology measurements
WO2020142301A1 (en) * 2019-01-02 2020-07-09 Kla Corporation Machine learning for metrology measurements
US20220318987A1 (en) * 2019-01-02 2022-10-06 Kla Corporation Machine Learning for Metrology Measurements
US11783466B2 (en) * 2019-01-02 2023-10-10 Kla Corporation Machine learning for metrology measurements
US11268805B2 (en) 2019-02-13 2022-03-08 Kioxia Corporation Measurement method
CN114503123A (en) * 2019-10-14 2022-05-13 科磊股份有限公司 Signal domain adaptation for metrology

Also Published As

Publication number Publication date
KR101059427B1 (en) 2011-08-25
US7831528B2 (en) 2010-11-09
CN1799045A (en) 2006-07-05
JP4589315B2 (en) 2010-12-01
CN100418083C (en) 2008-09-10
WO2005003911A2 (en) 2005-01-13
KR20060033740A (en) 2006-04-19
DE112004001001T5 (en) 2006-09-14
JP2007528985A (en) 2007-10-18
WO2005003911A3 (en) 2005-06-30
US20090198635A1 (en) 2009-08-06

Similar Documents

Publication Publication Date Title
US7831528B2 (en) Optical metrology of structures formed on semiconductor wafers using machine learning systems
US7523076B2 (en) Selecting a profile model for use in optical metrology using a machine learning system
US7453584B2 (en) Examining a structure formed on a semiconductor wafer using machine learning systems
TWI509431B (en) Method for automated determination of an optimally parameterized scatterometry model
US7372583B1 (en) Controlling a fabrication tool using support vector machine
CN107092958B (en) Accurate and fast neural network training for library-based critical dimension CD metrology
US7523021B2 (en) Weighting function to enhance measured diffraction signals in optical metrology
KR101144402B1 (en) Method and system of selecting a hypothetical profile to use in optical metrology, and computer readable storage medium therefor
EP1541960A2 (en) Parametric optimization of optical metrology model
US20130110477A1 (en) Process variation-based model optimization for metrology
US20130158957A1 (en) Library generation with derivatives in optical metrology
US7483809B2 (en) Optical metrology using support vector machine with profile parameter inputs
US10386729B2 (en) Dynamic removal of correlation of highly correlated parameters for optical metrology
CN106030282B (en) Method for automatic wavelength or angle pruning for optical metrology and optical system
US7522295B2 (en) Consecutive measurement of structures formed on a semiconductor wafer using a polarized reflectometer
US7511835B2 (en) Optical metrology using a support vector machine with simulated diffraction signal inputs
US7446887B2 (en) Matching optical metrology tools using hypothetical profiles
US7446888B2 (en) Matching optical metrology tools using diffraction signals
KR101179300B1 (en) Examining a structure formed on a semiconductor wafer using machine learning systems

Legal Events

Date Code Title Description
AS Assignment

Owner name: TIMBRE TECHNOLOGIES, INC., CALIFORNIA

Free format text: ASSIGNMENT OF ASSIGNORS INTEREST;ASSIGNORS:DODDI, SRINIVAS;DREGE, EMMANUEL;JAKATDAR, NICKHIL;AND OTHERS;REEL/FRAME:014257/0857

Effective date: 20030627

AS Assignment

Owner name: TOKYO ELECTRON LIMITED, JAPAN

Free format text: ASSIGNMENT OF ASSIGNORS INTEREST;ASSIGNOR:TIMBRE TECHNOLOGIES, INC.;REEL/FRAME:022388/0109

Effective date: 20090312

STCB Information on status: application discontinuation

Free format text: ABANDONED -- FAILURE TO RESPOND TO AN OFFICE ACTION