Library accuracy enhancement and evaluation

[0001] 1. Field

[0002] The present application generally relates to optical metrology, and, more particularly, to evaluating and enhancing a library generated using a machine learning system.

[0003] 2. Description of the Related Art

[0004] In semiconductor manufacturing, periodic gratings are typically used for quality assurance. For example, one typical use of periodic gratings includes fabricating a periodic grating in proximity to the operating structure of a semiconductor chip. The periodic grating is then illuminated with an electromagnetic radiation. The electromagnetic radiation that deflects off of the periodic grating are collected as a diffraction signal. The diffraction signal is then analyzed to determine whether the periodic grating, and by extension whether the operating structure of the semiconductor chip, has been fabricated according to specifications.

[0005] In one conventional system, the diffraction signal collected from illuminating the periodic grating (the measured-diffraction signal) is compared to a library of simulated-diffraction signals. Each simulated-diffraction signal in the library is associated with a hypothetical profile. When a match is made between the measured-diffraction signal and one of the simulated-diffraction signals in the library, the hypothetical profile associated with the simulated-diffraction signal is presumed to represent the actual profile of the periodic grating.

[0006] The library of simulated-diffraction signals can be generated using rigorous method, such as rigorous coupled wave analysis (RCWA). More particularly, in the diffraction modeling technique, a simulated-diffraction signal is calculated based, in part, on solving Maxwell's equations. Calculating the simulated diffraction signal involves performing a large number of complex calculations, which can be time consuming and costly.

[0007] An alternative is to generate the library of simulated-diffraction signals using a machine learning system (MLS). Prior to generating the library of simulated-diffraction signals, the MLS is trained using know input and output data. For a library generated using MLS, it is desirable to evaluate the accuracy of the trained system, especially near the boundaries of the library. In particular, as the critical dimension (CD) measured using metrology decreases, it is desirable to increase the accuracy of the library. Additionally, it is desirable to minimize the amounts of information stored in the library.

[0008] In one exemplary embodiment, the accuracy of a library of simulated-diffraction signals for use in optical metrology of a structure formed on a wafer is evaluated by utilizing an identity relationship inherent to simulated diffraction signals. Each simulated diffraction signal contains at least one set of four reflectivity parameters for a wavelength and/or angle of incidence. One of the four reflectivity parameters is selected. A value for the selected reflectivity parameter is determined using the identity relationship and values of the remaining three reflectivity parameters. The determined value for the selected reflectivity parameter is compared to the value in the obtained set of four reflectivity parameters to evaluate and improve the accuracy of the library. The identity relationship can also be used to reduce the data storage in a library.

[0018] 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.

1. Optical Metrology

[0019] With reference to FIG. 1, an optical metrology system 100 can be used to examine and analyze a structure. For example, optical 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.

[0020] As depicted in FIG. 1, optical metrology system 100 can include an optical 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 θ_i with respect to normal 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 θ_d with respect to normal, 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.

[0021] Optical 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.

2. Library-Based Process

[0022] In a library-based process, the measured diffraction signal is compared to a library of simulated diffraction signals. More specifically, each simulated diffraction signal in the library is associated with a hypothetical profile of the structure. When a match is made between the measured diffraction signal and one of the simulated diffraction signals in the library or when the difference between the measured diffraction signal and one of the simulated diffraction signals in the library is within a preset or matching criterion, the hypothetical profile associated with the matching simulated diffraction signal in the library is presumed to represent the profile of the structure. Thus, in this manner, a feature of the structure can be determined based on the hypothetical profile associated with the matching simulated diffraction signal.

[0023] With reference again to FIG. 1, after obtaining a measured diffraction signal, processing module 114 compares the measured diffraction signal to simulated diffraction signals stored in a library 116. Each simulated diffraction signal in library 116 is associated with a hypothetical profile. When a match is made between the measured diffraction signal and one of the simulated diffraction signals in library 116, the hypothetical profile associated with the matching simulated diffraction signal in library 116 can be presumed to represent the profile of periodic grating 102.

[0024] The set of hypothetical profiles stored in library 116 can be generated by characterizing a hypothetical profile using a set of parameters, then varying the set of parameters to generate hypothetical profiles of varying shapes and dimensions. The process of characterizing a hypothetical profile using a set of parameters can be referred to as parameterizing.

[0025] For example, as depicted in FIG. 2A, assume that hypothetical 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 hypothetical profile 200 can be characterized by increasing the number of parameters. For example, as depicted in FIG. 2B, hypothetical 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 hypothetical 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 hypothetical profile 200, including angle of incident (AOI), pitch, n & k, hardware parameters (e.g., polarizer angle), and the like.

[0026] As described above, the set of hypothetical profiles stored in library 116 (FIG. 1) can be generated by varying the parameters that characterize the hypothetical 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.

[0027] Thus, the parameters of the hypothetical profile associated with a matching simulated diffraction signal can be used to determine a feature of the structure being examined. For example, a parameter of the hypothetical profile corresponding to a bottom CD can be used to determine the bottom CD of the structure being examined.

[0028] With reference again to FIG. 1, the number of hypothetical profiles and corresponding simulated diffraction signals in the set of hypothetical profiles and simulated diffraction signals stored in library 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 hypothetical profiles and the simulated 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.

[0029] 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.

3. Machine Learning Systems

[0030] With reference to FIG. 1, in one exemplary embodiment, a MLS 118 can be used to examine a structure formed on a semiconductor wafer. MLS 118 employs a machine learning algorithm, such as back-propagation, radial basis function, support vector, kernel regression, and the like. For a more detailed description of MLS and machine learning algorithms, see “Neural Networks” by Simon Haykin, Prentice Hall, 1999, which is incorporated herein by reference in its entirety.

[0031] In the present exemplary embodiment, MLS 118 has been trained to receive a hypothetical profile as an input and generate a simulated diffraction signal as an output. Although in FIG. 1 MLS 118 is depicted as a component of processing module 114, it should be recognized that MLS 118 can be a separate module. It should be recognized that processing module 114 need not include both library 116 and MLS 118.

[0032] FIG. 3 depicts an exemplary process 300 for using a MLS to examine a structure formed on a semiconductor wafer. In 302, a measured diffraction signal of the structure is obtained by using an optical metrology device. In 304, after the MLS has been trained, a simulated diffraction signal is generated using the MLS. In 306, the measured and simulated diffraction signals are compared. In 308, a feature of the structure is determined based on the comparison of the measured and simulated diffraction signals.

[0033] More particularly, as described above, a hypothetical profile is used as an input to the MLS to generate the simulated diffraction signal. The hypothetical profile is characterized by one or more parameters. Thus, when the simulated diffraction signal matches the measured diffraction signal within a matching criterion, the hypothetical profile, and thus the one or more parameters that characterize the hypothetical profile, can be used to determine a feature of the structure.

[0034] When the simulated diffraction signal does not match the measured diffraction signal within a matching criterion, another hypothetical profile is used as an input to the MLS to generate another simulated diffraction signal. This new simulated diffraction signal is then compared with the measured diffraction signal. This process can be iterated until a simulated diffraction signal is generated that matches the measured diffraction signal within the matching criterion.

[0035] With reference to FIG. 1, in one exemplary embodiment, an MLS is used to generate a library of simulated diffraction signals and hypothetical profiles. In particular, the simulated diffraction signals in the library are generated using the MLS.

[0036] In particular, a set of hypothetical profiles to be included in the library are inputted into the MLS, which then generates a set of simulated diffraction signals corresponding to the set of hypothetical profiles. A hypothetical profile and the corresponding simulated diffraction signal generated for the hypothetical profile using the MLS is stored as a hypothetical profile and simulated diffraction signal pair in the library. In this manner, each of the hypothetical profiles in the set of hypothetical profiles and each of the simulated diffraction signals in the set of simulated diffraction signals are stored as hypothetical profile and diffraction signal pairs in the library.

[0037] With reference to FIG. 4, an exemplary process 400 is depicted for using a MLS in a library-based process. In 402, a library of simulated diffraction signals is generated using the MLS. More particularly, the library of simulated diffraction signals is generated by inputting a set of hypothetical profiles into the MLS. In 404, a measured diffraction signal is obtained using a metrology device, such as an ellipsometer, reflectometer, and the like. In 406, the measured diffraction signal is compared to the simulated diffraction signals in the library of simulated diffraction signals generated using the MLS. In 408, a feature of the structure is determined using the hypothetical profile corresponding to the matching simulated diffraction signal from the library of simulated diffraction signals.

[0038] For a more detailed description of generating a library of simulated diffraction signals using MLS see U.S. patent application Ser. No. 10/608,300, titled OPTICAL METROLOGY OF STRUCTURES FORMED ON SEMICONDUCTOR WAFERS USING MACHINE LEARNING SYSTEMS, filed on Jun. 27, 2003, which is hereby incorporated by reference in its entirety.

4. Library Accuracy Enhancement and Evaluation

[0039] In one exemplary embodiment, optical information from the simulated diffraction signals generated by the MLS to create a library of simulated diffraction signals can be used to test the accuracy of the library of simulated diffraction signals.

[0040] Light at a given wavelength and angle of incidence which scatters off a classical grating mount has two independent complex reflectance parameters contained within the diffraction signal, r_s and r_p, which can be used to describe the interaction of the light with the grating. The intensity of the reflected light is related to the complex reflectance parameters according to the following relationship:

[0041] $\begin{array}{cc}{I}_{\mathrm{out}}\propto {E_{\mathrm{out}}}^2=\frac{1}{2}{I}_{\mathrm{in}}f\left({r_s}^2+{r_p}^2\pm 2\mathrm{Re}\left(r_s{r}_p^{*}{e}^{i\varphi }\right)\right).& \left(1\right)\end{array}$
f(|r_s|²+|r_p|²±2 Re(r_sr_p*e^iφ)) is a function which describes the effect of the reflecting surface on the incident beam I_in I_out is the intensity of the reflected light beam, for a give wavelength and angle of incidence. E_out is the electric field of the reflected beam. φ is the common phase between the complex reflectance parameters.

[0042] When the incident beam is linearly polarized at a 45° angle relative to the plane of incidence equation (1) simplifies to the following:

[0043] $\begin{array}{cc}{I}_{\mathrm{out}}\propto {E_{\mathrm{out}}}^2=\frac{1}{2}{I}_{\mathrm{in}}\left({r_s}^2+{r_p}^2\pm 2\mathrm{Re}\left(r_s{r}_p^{*}{e}^{i\varphi }\right)\right).& \left(2\right)\end{array}$
If φ is 0 or π, then equation (2) further simplifies to:

[0044] $\begin{array}{cc}{I}_{\mathrm{out}}\propto {E_{\mathrm{out}}}^2=\frac{1}{2}{I}_{\mathrm{in}}\left({r_s}^2+{r_p}^2\pm 2\mathrm{Re}\left(r_s{r}_p^{*}\right)\right).& \left(3\right)\end{array}$
If φ is π/2 or 3π/2, then equation (2) further simplifies to:

[0045] $\begin{array}{cc}{I}_{\mathrm{out}}\propto {E_{\mathrm{out}}}^2=\frac{1}{2}{I}_{\mathrm{in}}\left({r_s}^2+{r_p}^2\pm 2\mathrm{Im}\left(r_s{r}_p^{*}\right)\right).& \left(4\right)\end{array}$

[0046] Thus, in order to generate a simulated diffraction signal for a given profile, four reflectivity parameters, |r_s|², |r_p|², Re(r_sr*_p), and Im(r_sr*_p), may be needed. Which parameters are needed will depend on the experimental design, for which the simulated diffraction signal is being generated.

[0047] Currently available optical metrology devices are typically sensitive only to |r_s|², |r_p|², and Re(r_sr*_p). They are not typically sensitive to Im(r_sr*_p), which represents the common phase of r_s and r_p. It can be shown that the four parameters, |r_s|², |r_p|², Re(r_sr*_p), and Im(r_sr*_p), are related through the following identity relationship:
Re(r_p*r_s)²+Im(r_p*r_s)²−|r_s|²×|r_p|²=0.  (5)
Thus, only |r_s|², |r_p|², and Re(r_sr*_p) may need to be measured, and then equation (5) used to calculate Im(r_sr*_p).

[0048] Given a hypothetical profile, a MLS can be trained to simulate the four reflectivity parameters, |r_p|², |r_s|², Re(r_p*r_s), and Im(r_p*r_s), for a given wavelength and/or incident angle. All four reflectivity parameters can be trained and stored as a whole or subgroups, such as group 1 of [|r_p|², |r_s|²] and group 2 of [Re(r_sr*_p), Im(r_sr*_p)]. Because of limitations present in a MLS used to generate each of the four reflectivity parameters, each individual reflectivity parameter may not be accurate. One such limitation is that the data used to train the MLS is not representative of the boundaries of the library, and may lead to larger errors in the four reflectivity parameters associated with the hypothetical profiles present in the boundary regions.

[0049] For example a few nm error for calculating the critical dimension of a trained set of data, which is fairly common with current MLS technologies, will propagate to much larger values near the boundaries of a library. These errors become more important for small critical dimension less than 70 nm. Thus, in one exemplary embodiment, the accuracy of the four reflectivity parameters simulated by the MLS can be tested using the identity relationship of the four reflectivity parameters (equation (5)).

[0050] In particular, in the present exemplary embodiment, an acceptance criterion can be set to ensure that the reflectivity parameters are accurate within the acceptance criterion. A value of one of the four reflective parameters is generated using the values of the remaining three reflectivity parameters from the four reflectivity parameters simulated by the MLS and the identity relationship of the four reflectivity parameters (equation (5)). For example, a value of the reflectivity parameter Im(r_sr*_p) can be generated using the values of |r_s|², |r_p|², and Re(r_sr*_p) from the four reflectivity parameters simulated by the MLS and the identity relationship of the four reflectivity parameters. The value of the reflectivity parameter generated using the identity relationship is then compared with the value of the corresponding reflectivity parameter of the four reflectivity parameters simulated by the MLS. For example, a value of the reflectivity parameter Im(r_sr*_p) generated using the identity relationship and a value of the reflectivity parameter Im(r_sr*_p) from the four reflectivity parameters simulated by the MLS are compared. If the two values of the reflectivity parameter Im(r_sr*_p) are not within the acceptance criterion, then the amount of error can be determined to be unacceptable.

[0051] With reference to FIG. 5, an exemplary process 500 is depicted for evaluating a library of simulated diffraction signals generated using a MLS. In 502, a library of simulated diffraction signals is obtained. In the present exemplary embodiment, the obtained library was generated using an MLS. More particularly, the library of simulated diffraction signals was generated by inputting a set of hypothetical profiles into the MLS to generate the set of simulated diffraction signals for the set of hypothetical profiles. A hypothetical profile and the corresponding simulated diffraction signal generated for the hypothetical profile using the MLS is stored as a hypothetical profile and simulated diffraction signal pair in the library. In this manner, each of the hypothetical profiles in the set of hypothetical profiles and each of the simulated diffraction signals in the set of simulated diffraction signals are stored as hypothetical profile and diffraction signal pairs in the library.

[0052] In 504, at least one of the simulated diffraction signals from the library is selected. In 506, at least one set of four reflectivity parameters for a given wavelength and/or angle of incidence is selected from the selected simulated diffraction signal. In 508, the at least one set of four reflectivity parameters is evaluated using the identity relationship of the four reflectivity parameters (equation (5)).

[0053] In 510, if the reflectivity parameters do not satisfy the identity relationship, then the library is determined to be unacceptable. In the present exemplary embodiment, the MLS is retrained and a new library of simulated diffraction signals is generated. The process is repeated until the at least one set of four reflectivity parameters satisfy the identity relationship.

[0054] In 512, if the four reflectivity parameters satisfy the identity relationship, then the library is determined to be acceptable. The library can then be used to evaluate structures formed on a semiconductor wafer.

[0055] With reference to FIG. 6, an exemplary process 600 is depicted for evaluating errors in the reflectivity parameters. In 602, the set of four reflectivity parameters that did not satisfy the identity relationship is obtained. In 604, an additional set of reflectivity parameters is generated using a rigorous method, such as RCWA. In 606, the values of the reflectivity parameters calculated using the MLS and the rigorous method, such as RCWA are compared. In 608, the errors in the MLS parameters are identified based on the comparison in 608. In 610, the information about the errors in the MLS parameters identified in 608 is used to retrain the MLS.

[0056] With reference to FIG. 7, a system, 700, for evaluating a library of simulated diffraction signals is depicted. The system includes a machine learning system 702 to generate a library of simulated diffraction signals 704. A selector 706 configured to select at least one set of four reflectivity parameters is connected to the library of diffraction signals 704.

[0057] Selector 706 is also connected to an evaluator 708. Evaluator 708 is configured to evaluate the at least one set of four reflectivity parameters according to the identity relationship (equation 5). Evaluator 708 can also be configured to generate at least one set of four reflectivity parameters using a rigorous method, such as RCWA. The set of four reflectivity parameters generated using the MLS and the set of four reflectivity parameters generated using RCWA can then be compared and used to evaluate the error in each of the individual reflectivity parameters.

[0058] Evaluator 708 is connected to a MLS trainer 710, which is configured to obtain error information from evaluator 708 and use that information to train MLS 702. MLS trainer 710 is also configured to initially train MLS 702 prior to generation of the initial library of simulated diffraction signals. A detailed description of generating a library of simulated diffraction signals using MLS is discussed in U.S. patent application Ser. No. 10/608,300, titled OPTICAL METROLOGY OF STRUCTURES FORMED ON SEMICONDUCTOR WAFERS USING MACHINE LEARNING SYSTEMS, filed on Jun. 27, 2003, which is hereby incorporated by reference in its entirety.

[0059] In one exemplary embodiment, the four reflectivity parameters for each wave length and incident angle of each simulated diffraction signal in the library are tested to see if they satisfy the identity relationship (equation 4). For example, following the generation of a library of simulated diffraction signals using a MLS, the sets of four reflectivity parameters for each wave length and incident angle of the simulated diffraction signals in the library are selected and evaluated using the identity relationship. An error for each set of four reflectivity parameters is then evaluated and grouped together to generate an error for the library of simulated diffraction signals as a whole. The error can then be used to decide if the MLS needs to be retrained and/or if the library of simulated diffraction signals needs to be generated. As described above, an acceptance criterion can be used to determine if the amount of error is acceptable.

[0060] In one exemplary embodiment, instead of using the four reflectivity parameters for each wave length and/or incident angle of each simulated diffraction signal in the library of simulated diffraction signals, a range of wave lengths and/or a range of incident angles of at least one simulated diffraction signal in the library are tested to see if they satisfy the identity relationship (equation 5). An amount of error can be calculated and used to evaluate the accuracy of the library of simulated diffraction signals.

[0061] In one exemplary embodiment, the four reflectivity parameters for each wavelength and/or angle of incidence for a range of simulated diffraction signals in the library are tested to see if they satisfy the identity relationship (equation 5). An amount of error can be calculated and used to evaluate the accuracy of the library of simulated diffraction signals.

[0062] In one exemplary embodiment, the four reflectivity parameters for each wavelength and/or angle of incidence for a random set of simulated diffraction signals in the library are tested to see if they satisfy the identity relationship (equation 5). An amount of error can be calculated and used to evaluate the accuracy of the library of simulated diffraction signals.

[0063] In one exemplary embodiment, the four reflectivity parameters for each wavelength and/or angle of incidence for a set of simulated diffraction signals present at the boundaries of the library are tested to see if they satisfy the identity relationship (equation 5). An amount of error can be calculated and used to evaluate the accuracy of the library of simulated diffraction signals.

5. Reduction in Data Stored in a Library

[0064] In one exemplary embodiment, the identity relationship (equation 5) can be used to reduce the complexity of a library of simulated diffraction signals generated using a MLS. The amount of data, N_d, which needs to be stored in a library of simulated diffraction signals can described by the following:
N_d=λ×P×AOI×4.  (6)
λ is the number of different wavelengths which make up the simulated diffraction signal. P is the number of hypothetical profiles in the library of simulated diffraction signals. AOI is the number of angle of incidences which make up the simulated diffraction signal.

[0065] The factor of 4 in equation 6 takes into account the four reflectivity parameters which are needed to calculate the simulated diffraction signal for a given wavelength and/or angle of incidence. Instead of training the library to store all four reflectivity parameters for a given wavelength and/or angle of incidence of a hypothetical profile, three of the four parameters can be trained and stored. This reduces the amount of data stored in the library by 25%. If the fourth reflectivity parameter is needed, then the identity relationship (equation 5) can be used to generate the fourth reflectivity parameters.

[0066] FIG. 8 depicts an exemplary process 800 for reducing the amount of data stored in a library of simulated diffraction signals. In 802, a set of simulated diffraction signals containing three of the four reflectivity parameters for each wavelength and/or angle incidence for a set of hypothetical profiles is generated using a MLS. In 804, the set of simulated diffraction signals and set of hypothetical profiles are stored in the library. In 806, the fourth reflectivity parameter for each wavelength and/or angle incidence for the set of diffraction signals is derived using the identity relationship (equation 5) and the three reflectivity parameters retrieved from the library.

[0067] Although exemplary embodiments have been described, various modifications can be made without departing from the spirit and/or scope of the present invention. Therefore, the present invention should not be construed as being limited to the specific forms shown in the drawings and described above.