The present invention relates generally to manufacture of semiconductor devices, and particularly to methods and target features for semiconductor circuit metrology.
Semiconductor circuits are commonly manufactured using photolithographic methods. In photolithography, a thin layer of a photosensitive polymer (photoresist) is deposited over a semiconductor substrate and patterned using optical or other radiation, leaving parts of the substrate covered by the photoresist. The photoresist is patterned by a scanner projecting an image of a reticle onto the photoresist, typically using ultraviolet radiation. After patterning, the substrate is modified by methods such as etching and ion bombardment to change the material properties and/or the topography of the substrate, while the parts of the substrate covered by the photoresist are not affected.
Semiconductor circuit metrology is used for measuring properties of the patterned photoresist, such as the topography and location of the patterned features. Accurate location of the patterned features of the photoresist with respect to previously patterned process layers is crucial for achieving a high yield of the photolithographic process. Any error in the registration (misregistration) of the patterned photoresist with respect to an underlying process layer is referred to as “overlay error.” As an example, in typical semiconductor circuits with minimum line-widths of 10-14 nm (so-called 10-nm design rule), the maximal permissible overlay error is 2-3 nm. In leading-edge semiconductor circuits, the line-widths are shrinking to 5 nm, with a concomitant reduction in maximal permissible overlay error.
Overlay error is commonly measured using optical overlay metrology apparatuses (commonly called optical overlay metrology tools), as optical radiation in the visible and infrared wavelengths is capable of penetrating through the photoresist layer, as well as through dielectric layers under the photoresist. Furthermore, infrared wavelengths are capable of penetrating a semiconductor substrate, such as silicon, enabling metrology through the substrate. The overlay error is measured from overlay targets located in the scribe lines of the semiconductor substrate (the lines separating adjacent dies) and/or within the dies.
Commonly used overlay metrology tools fall into one of two categories: scatterometry tools and imaging tools. Scatterometry tools, such as the ATL100™ tool by KLA Corporation (Milpitas, CA, USA), capture a diffracted (scatterometric) image of periodic target features of the overlay target from the exit pupil of the objective lens of the metrology tool. The scatterometric image, indicative of the angular distribution of the optical radiation that is scattered from the target features, is processed in order to measure the overlay error.
Imaging tools, such as the Archer™-series tools by KLA Corporation (Milpitas, CA, USA), image an overlay target, such as AIM™ overlay target by KLA. An image analysis algorithm is applied to the acquired images in order to locate the center of symmetry of the target features in the process layer and the center of symmetry of the target features in the photoresist layer. The overlay error is computed based on the displacement between the centers of symmetry of the target features in the two layers.
The terms “optical radiation” and “light,” as used in the present description and in the claims, refer generally to any and all of visible, infrared, and ultraviolet radiation.
Embodiments of the present invention that are described hereinbelow provide improved methods and systems for metrology using overlay targets, as well as targets for use in such methods.
There is therefore provided, in accordance with an embodiment of the invention, a method for semiconductor metrology. The method includes depositing a first film layer on a semiconductor substrate and a second film layer overlying the first film layer, and patterning the first and second film layers to define a first overlay target and a second overlay target. The first overlay target is disposed in a first location on the semiconductor substrate and includes a first target feature formed in the first film layer and a second target feature formed in the second film layer in a position adjacent to the first target feature. The second overlay target is disposed in a second location on the semiconductor substrate and includes a first part, which is identical to the first overlay target, and a second part, which is disposed adjacent to the first part such that the second overlay target has rotational symmetry of 180° around a normal to the semiconductor substrate. The method further includes capturing a first image, using an imaging assembly, of the second overlay target, processing the first image to compute a target calibration function based on both the first and second parts of the second overlay target, capturing a second image, using the imaging assembly, of the first overlay target, and processing the second image while applying the target calibration function to estimate an overlay error between the patterning of the first and second film layers at the first location.
In some embodiments, the second part of the second overlay target includes a rotated copy of the first part.
In additional embodiments, the first overlay target is one of a plurality of first overlay targets, each including the first and second target features, disposed at different, respective locations on the semiconductor substrate, and processing the second image includes applying the target calibration function to each of the first overlay targets.
In further embodiments, processing the first image includes using both the first and second parts of the second overlay target in the first image to estimate a first overlay error between the patterning of the first and second film layers, using only the first part of the second overlay target to estimate a second overlay error between the patterning of the first and second film layers, and computing the target calibration function responsively to a difference between the first and the second overlay errors.
In yet further embodiments, using both the first and second parts includes estimating the first overlay error by finding a displacement between respective first centers of symmetry of the first target features and the second target features in both the first and second parts of the second overlay target, and using only the first part includes estimating the second overlay error by finding a displacement between respective second centers of symmetry of the first target features and the second target features in only the first part of the second overlay target.
In some embodiments, the first image is captured in a first orientation of the semiconductor substrate, and the method includes capturing a third image of the second overlay target in a second orientation of the semiconductor substrate, which is rotated by 180° about a normal to the substrate relative to the first orientation, and processing the first image includes processing both the first and third images to estimate respective first and second overlay errors in the first and second orientations, and computing the target calibration function based on the first and second overlay errors.
In additional embodiments, the semiconductor substrate includes dies separated by scribe lines, and the first overlay target is disposed in a device area of a die and the second overlay target is disposed in a scribe line.
In further embodiments, the first target feature includes a first linear grating oriented along a first direction in the first film layer, and the second target feature includes a second linear grating oriented in the first direction in the second film layer.
In additional embodiments, the first target feature further includes a third linear grating oriented along a second direction, which is not parallel to the first direction, in the first film layer, and the second target feature includes a fourth linear grating oriented in the second direction in the second film layer.
In some embodiments, the method includes measuring an angular misalignment of the semiconductor substrate, wherein applying the target calibration function includes correcting for the angular misalignment in estimating the overlay error.
In additional embodiments, the first overlay target is one of a plurality of first overlay targets disposed at different, respective locations on the semiconductor substrate, and measuring the angular misalignment includes estimating and compensating for a local angular misalignment at each of the different locations.
There is also provided, in accordance with an embodiment of the invention, a product, which includes a semiconductor substrate and first and second film layers, which are disposed on the substrate with the second film layer overlying the first film layer. The first and second film layers are patterned to define a first overlay target and a second overlay target. The first overlay target is disposed in a first location on the semiconductor substrate and includes a first target feature formed in the first film layer and a second target feature formed in the second film layer in a position adjacent to the first target feature. The second overlay target is disposed in a second location on the semiconductor substrate and includes a first part, which is identical to the first overlay target, and a second part, which is disposed adjacent to the first part such that the second overlay target has rotational symmetry of 180° around a normal to the semiconductor substrate.
There is further provided, in accordance with an embodiment of the invention, an apparatus for semiconductor metrology. The apparatus includes an imaging assembly, which is configured to capture images of a semiconductor substrate on which first and second film layers are disposed, with the second film layer overlying the first film layer. The first and second film layers are patterned to define a first overlay target and a second overlay target. The first overlay target is disposed in a first location on the semiconductor substrate and includes a first target feature formed in the first film layer and a second target feature formed in the second film layer in a position adjacent to the first target feature. The second overlay target is disposed in a second location on the semiconductor substrate and includes a first part, which is identical to the first overlay target, and a second part, which is disposed adjacent to the first part such that the second overlay target has rotational symmetry of 180° around a normal to the semiconductor substrate. The apparatus further includes a processor, which is configured to process a first image captured by the imaging assembly of the second overlay target to compute a target calibration function based on both the first and second parts of the second overlay target, and to process a second image captured by the imaging assembly of the first overlay target while applying the target calibration function to estimate an overlay error between the patterning of the first and second film layers at the first location.
The present invention will be more fully understood from the following detailed description of the embodiments thereof, taken together with the drawings in which:
Overlay targets for overlay metrology are commonly used for precise and accurate measurements of the overlay error between successive patterned layers on a semiconductor substrate. These layers may comprise, for example, a process layer and a photoresist layer (photoresist), or, in after-etch applications, two process layers. Thus, although some example embodiments are described below with reference to a process layer and a photoresist layer, the principles of these embodiments may be applied, mutatis mutandis, to a first process layer and a second process layer. In some multiple patterning applications, the first and second process layers may comprise the same material. In some multilayer applications, the layers in which the target features of an overlay target are formed may comprise more than two layers.
Commonly used imaging overlay targets have typical dimensions of 20 μm×20 μm. Due their relatively large size, they cannot be located within the functional device area of the semiconductor circuits formed on the dies defined on a substrate, but are rather located in the scribe lines separating adjacent dies. In embodiments of the present invention, to measure the overlay error within the device area, smaller targets may be placed in this area. These smaller targets are referred to herein as “half-targets”, because they comprise only a subset of the target features of the full overlay targets in the scribe lines.
However, a single overlay measurement using a half-target may suffer from metrology errors due to at least the following three error sources: 1) angular misalignment of the half-target with respect to the Cartesian coordinates in which the overlay error is expressed, 2) aberrations of the optics of the overlay metrology tool, and 3) uncertainty regarding the actual optical magnification of the overlay tool. As the half-targets do not possess 180° rotational symmetry (in contrast to the full targets) , calibration of the metrology errors of these half-targets, which is commonly performed on full targets by measuring the target at two rotational orientations 180° apart, is not feasible.
The embodiments described hereinbelow address the problem of calibrating the metrology errors of half-targets using full targets on the same substrate. Each such full target comprises a half-target and is complemented by an additional target structure so that the full target is symmetrical over a 180° rotation. In one embodiment, such a full target comprises a half target together with a copy of the half target, wherein the copy is rotated around a normal to the substrate by 180° with respect to the non-rotated half-target. In alternative embodiments, the additional target structure may be different from the half-target.
To derive the parameters of a calibration function for the half-targets, overlay error is measured from a full target in two ways:
In additional embodiments, a measured angular misalignment of the substrate is used for correcting for angular misalignment of the overlay target, as an additional correction to the overlay target calibration function described hereinabove. Alternatively, this technique for correction of angular misalignment may be used independently of the overlay target calibration function.
In the disclosed examples, a method for semiconductor metrology comprises depositing a first film layer on a semiconductor substrate and a second film layer overlying the first film layer. The first and second film layers are patterned to define a half-target in a first location on the semiconductor substrate (for example in the device area) and a full target in a second location (for example in the scribe line). The half-target comprises a first target feature formed in the first film layer and a second target feature formed in the second film layer in a position adjacent to the first target feature. In some embodiments, the full target comprises a first part, which is identical to the half-target, and a second part, which comprises a rotated copy of the first part. The second part is disposed adjacent to the first part such that the full target has rotational symmetry of 180° around a normal to the semiconductor substrate. Alternatively, other full target designs may be used as long as they contain the half-target and have rotational symmetry of 180° around the normal.
An imaging assembly captures images of the half and full targets. The image of the full target is processed to compute a target calibration function based on both the first and second parts of the full target. The image of the half-target is processed, while applying the target calibration function, to estimate the overlay error between the patterning of the first and second film layers at the location of the half-target.
Overlay Metrology Apparatus
Imaging overlay metrology apparatus 10 comprises an imaging assembly 14, an illumination assembly 16, a controller 18, and a table 20 on which wafer 12 is mounted. Imaging assembly 14 comprises an objective lens 22, a cube beamsplitter 24, and an imaging lens 26. Imaging assembly 14 further comprises a two-dimensional sensor array 28, comprising for example, a complementary metal-oxide- semiconductor (CMOS) detector with a two-dimensional array of pixels 30. Imaging lens 26 images the top surface of wafer 12 onto sensor array 28.
Illumination assembly 16 comprises a light source 32, emitting optical radiation, and a lens 34. Table 20 is located in proximity to objective lens 22, and comprises actuators, controlled by controller 18, which can move the table linearly in the x-, y-, and z-directions (with reference to Cartesian coordinates 36), as well as rotate the table around the z-axis.
In the pictured embodiment, a first film layer 38 has been deposited over semiconductor wafer 12 and patterned in a photolithographic process. In a subsequent process step, a second film layer 40, comprising photoresist, has been deposited over first film layer 38. In the present embodiment, first film layer 38 is referred to as a “process layer, ” and second film layer 40 is referred to as a “photoresist layer.” In alternative embodiments, such as after-etch applications, both the first and second film layers may comprise process layers. Layers 38 and 40 comprise patterns of semiconductor circuits, as well as of overlay targets, formed by a photolithographic process.
Controller 18 is coupled to sensor array 28 and to table 20. Controller 18 typically comprises a programmable processor, which is programmed in software and/or firmware to carry out the functions that are described herein, along with suitable digital and/or analog interfaces for connection to the other elements of apparatus 10. Alternatively or additionally, controller 18 comprises hard-wired and/or programmable hardware logic circuits, which carry out at least some of the functions of the controller. Although controller 18 is shown in
To capture an image of an overlay target in film layers 38 and 40, wafer 12 is positioned on table 20 so that the target is in the field of view (FOV) of objective lens 22. Light source 32 projects a beam of optical radiation to lens 34, which further projects the beam to cube beamsplitter 24. Beamsplitter 24 reflects the beam into objective lens 22, which projects the beam onto wafer 12 illuminating the overlay target. The radiation impinging on wafer 12 is reflected back to objective lens 22, and further imaged by lens 26 onto sensor array 28. Controller 18 captures the image and processes it in order to measure the overlay error.
Half-Targets
Half-target 100 comprises a process grating 104 as a first target feature, formed in process layer 38, and a photoresist grating 106 as a second target feature, formed in photoresist layer 40. Each grating comprises six parallel, equispaced and equal-width bars oriented in the y-direction. In the pictured example, the photoresist grating is located above the process grating (i.e., in the positive direction along the y-axis). Because this arrangement is non-symmetrical, other, similar half-targets (not shown) may be formed on the semiconductor substrate with the process grating above the photoresist grating.
In an ideal lithographic process, the bars of the two gratings 104 and 106 will be aligned with each other in the x-direction, corresponding to a nominal x-overlay error of zero. (In the present description, the term “nominal” refers to the dimensions and patterns that would be printed in an ideal lithographic process, in accordance with the design of the masks used to pattern the two film layers.) However, due to process and lithography errors, gratings 104 and 106 are shifted with respect to each other in the x-direction by the amount of the x-overlay error, labeled OVLx. (For the sake of clarity, the shift between process grating 104 and photoresist grating 106 has been exaggerated in the figure.)
For measuring the overlay error in the x-direction using half-target 100, two regions of interest (ROI) 108 and 110 are defined over process grating 104 and photoresist grating 106, respectively. (Although ROIs 108 and 110 are shown in the figures as encompassing the entire half-targets, smaller ROIs, containing only parts of the half-targets, may alternatively be used.) Half-target 100 is imaged onto sensor array 28 (
Similarly to half-target 100, half-target 102 comprises a process grating 122 as a first target feature, formed in process layer 38, and a photoresist grating 124 as a second target feature, formed in photoresist layer 40, with each grating comprising six parallel bars. However, gratings 122 and 124 are positioned side-by-side in the x-direction, rather than in the y-direction as in half-target 100. For measuring the overlay error in the x-direction using half-target 102, two ROIs 126 and 128 are defined over process grating 122 and photoresist grating 124, respectively. Again similarly to half-target 100, positions of centers of symmetry 130 and 132 are computed by controller 18 from a captured image of half-target 102, and projected onto an x-axis 134 to respective projections 136 and 138 with a spacing Δx. However, unlike the spacing between projections 118 and 120 for half-target 100, spacing Δx is a sum of the nominal x-distance Dnominal,x between centers of symmetry 130 and 132 and the overlay error OVLx: Δx=Dnominal,x+OVLx. Thus, the overlay error is computed by subtracting Dnominal,x from the measured spacing Δx: OVLx=Δx−Dnominal,x.
For measuring the overlay error in the y-direction, half-targets similar to half-targets 100 and 102 may be used with a 90° rotation of these targets.
Although half-targets 100 and 102 are shown in the figures as comprising gratings of six parallel bars, in alternative embodiments gratings with fewer or more bars may be used. In yet other embodiments, the first target feature in process layer 38 and the second target feature in photoresist layer 40 may comprise any other pattern satisfying the following conditions of symmetry: A target feature used for measuring x-overlay error should have reflection symmetry about the y-axis, and a target feature used for measuring y-overlay error should have reflection symmetry about the x-axis. Alternatively, one or each of these target features should by symmetrical around a 180° rotation around the z-axis. Moreover, the first and second target features may differ from each other, as long as the above symmetry conditions are satisfied.
Alternatively, the half-targets may comprise Moiré-targets, wherein each of the first and second target features comprises a linear photoresist grating overlaid on a process grating. For each target feature, the two gratings have a slightly differing spatial frequencies, so that the captured image has a spatial frequency equal to the difference between the grating frequencies. By designing the two target features to have spatial frequency differences that are equal in magnitude but with opposite signs, controller 18 can process the captured images of the first and second target features to estimate the overlay error between process layer 38 and photoresist layer 40.
Half-target 200 comprises four target features 204, 206, 208, and 210. Each of target features 204 and 206 comprises six parallel bars oriented in the y-direction, similar to target features 122 and 124 of half-target 102 (
Although the bars of target features 204, 206, 208, and 210 are aligned in the figure along the Cartesian x-and y-axes, in an alternative embodiment this alignment may be relaxed. For example, the bars of target features 208 and 210 may be oriented in another direction, as long as this direction is not parallel with the y-direction.
Half-target 202 comprises target features 212 and 214, wherein each target feature comprises two target features of half-target 200 in an overlaid “hatched” configuration. Thus, target feature 212 comprises target features 206 and 208 from half-target 200, and target feature 214 comprises target features 204 and 210. For estimating x- and y-overlay errors from half-target 202, controller 18 identifies the bars in the two orthogonal directions in the captured images of each of target features 212 and 214, and then use the methods described hereinabove.
Similarly to
Error Sources for Half-Targets 100 And 102
Half-target 220 is similar to half-target 100 (
Similarly to measuring overlay error using half-target 100, two ROIs 226 and 228 are defined over process grating 222 and photoresist grating 224, respectively. Controller 18 captures images of gratings 222 and 224 within ROIs 226 and 228, and computes respective centers of symmetry 230 and 232. Centers of symmetry 230 and 232 are projected (in Cartesian coordinates 36) to respective projections 234 and 236 on an x-axis 238, wherein the distance between these two projections, Δangular, is due entirely to the angular misalignment α of half-target 220. Were the distance between projections 234 and 236 taken as the measured x-overlay error OVLx, this result would be in error by the amount of Δangular.
The error Δangular, due to pivoting of centers of symmetry 230 and 232 along the x-direction, may be computed as Δangular=α×DROI,y, where DROI,y is the separation between centers of symmetry 230 and 232 in the y-direction, i.e., the separation between the centers of the two ROIs 226 and 228. (As angular misalignments of this sort are usually very small, such as a few milliradians, small-angle approximations are used in the description.) For example, using values of DROI,y=5 μm and α=1 mrad leads to an error of Aangular=5 nm.
Similar errors, due to angular misalignment, will affect the measured overlay errors when using two-dimensional half-targets, such as half-target 200 (
Optical aberrations of the overlay metrology tool may lead to a shift of the bars of gratings 104 and/or 106 of half-target 100 in the x-direction, potentially even in mutually opposite directions. The aberrations may consequently affect the measured displacements of the gratings in the x-direction, and thus the measured x-overlay error. A similar shift of the bars of gratings 122 and/or 124 of half-target 102 may affect the measured displacements of the gratings.
An uncertainty of the actual optical magnification M of the overlay metrology tool by AM may lead to an error ΔMag for the nominal x-distance Dnominal,x between centers of symmetry 130 and 132 in half-target. 102 (
Similar errors due to uncertainty of the actual optical magnification M may be experienced when using two-dimensional half-targets, such as half-target 200 (
The rotational symmetry of full targets 300 and 302 makes it possible for apparatus 10 to measure the overlay error accurately by capturing and processing images of the target at relative rotations of 0° and 180°. This method enables the tool-induced shift (TIS), due to inaccuracies in the metrology apparatus, to be calibrated and thus separated from the actual overlay error. Thus, the term “accurate” is used in the present description to refer to TIS-calibrated overlay measurements.
As will be detailed below, full target 300 may be used to measure the x-overlay error accurately, as well as to calibrate the x-overlay error measured using half-target 100. Full target 302 may be used to measure the overlay error accurately in both x and y-directions, as well as to calibrate x- and y-overlay errors measured using half-target 200.
Calibrating Half-Target 100 Using Full Target 300
Full target 300 comprises a first part 304 and a second part 306, wherein the first part is identical to half-target 100 and the second part is a copy of half-target 100 rotated by 180° around the normal to substrate 12 (around the z-axis). Full target 300 thus comprises a first target pattern formed by process layer gratings 308 and 310 and a second target pattern formed by photoresist layer gratings 312 and 314.
Using full target 300, x-overlay error is measured independently in two orientations of semiconductor substrate 12 that are 180° apart. In the first orientation, referred to as the 0°-orientation, an x-overlay error OVLx,0 is measured. To measure the position of a first center of symmetry 316 of the first target pattern, two ROIs 318 and 320 are defined over respective process layer gratings 308 and 310 in an image of full target 300 captured by apparatus 10 (
Controller 18 similarly finds the position of a second center of symmetry for the second target pattern by processing the image within two ROIs positioned over photoresist gratings 312 and 314. (For the sake of simplicity, the second center of symmetry and the corresponding ROIS are omitted from the figure.) Controller 18 estimates OVLx,0 as the separation between first and second centers of symmetry.
After a 180° rotation of semiconductor substrate 12 around its normal, an x-overlay error OVLx,180 is measured using the same method as for measuring OVLx,0. Controller 18 computes an accurate x-overlay error OVLx,ACC as half of the difference between the x-overlay errors measured in the two substrate orientations: OVLx,ACC=(OVLx,0−OVLx,180)/2.
Alternatively, the measurement of the overlay error in 180° orientation may be omitted, and the overlay error OVLx,0 may be used as OVLx,ACC in the computations hereinbelow.
To calibrate half-target 100 (as shown in
A calibration for measuring y-overlay error using one-dimensional half-targets is done in a similar way.
Full target 302 (
Using full target 302, both x- and y-overlay errors are measured in two orientations of semiconductor substrate that are 180° apart. In the first, 0°-orientation, overlay errors OVLx,0 and OVLy,0 are measured. In the second, 180°-orientation, overlay errors OVLx,180 and OVLy,180 are measured. The overlay errors are measured in the manner described above with reference to full target 300, with x-overlay measurements using gratings 334, 336, 342, and 344, and y-overlay measurements using gratings 338, 340, 346, and 348. Accurate overlay errors are computed similarly to OVLx,ACC hereinabove:
For calibrating overlay error measurements using half-target 200, x- and y-overlay errors OVLx,HT and OVLy,HT are measured using only first part 330, which is identical to half-target 200. Thus, the same method is used as that used to measure x- and y-overlay errors OVLx, and OVLy for half-target 200 in
Similarly to the calibration of half-target 100 using full target 300, described hereinabove, the two-component target calibration function (ΔCAL,x, ΔCAL,y) may be either computed by controller 18 in the beginning of the overlay error metrology process and applied to overlay errors as they are measured, or it may be computed independently of the sequence of overlay error measurements, and applied to the measured overlay errors at the end of the sequence.
In a full target selection step 402, controller 18 selects a full target FTi for the calibration process, wherein i is an index used to enumerate full targets for a multi-target calibration (reduction of target-to-target variations). In a measurement start step 404, a jth measurement of full target FTi is started (j is an index used to enumerate repeated measurements of a given target for improving measurement repeatability).
In a measurement step 406, controller 18 measures an accurate x-overlay error OVLx,ACCij based on the measurement initiated at step 404. This step, as well as the subsequent steps in flowchart 400, is similar to the calibration technique described above for full target 300 in
In a first decision step 414, controller 18 decides whether to repeat the measurements on full target FTi for increased repeatability. This decision may be taken by controller 18 either by computing the repeatability from the first j measurements or by using a preset count for the number of measurements. If the measurement is to be repeated, the index j is incremented in a first incrementation step 416, and the process returns to step 404. When no additional measurements of full target FTi are required, the process continues to a second target calibration function step 418, wherein the acquired target calibration functions ΔACAL,xij for full target FTi are averaged to give the value ΔCAL,xi for full target i.
The process continues to a second decision step 420, wherein controller 18 decides whether to include additional full targets in the calibration process in order to mitigate target-to-target variations. The decision in step 420 may be taken by controller 18 either by estimating the target-to-target variation from the first i full targets, by using a preset count for the number of full targets to be included, or by using a preset list of full targets on semiconductor substrate 12. When additional full targets are to be included, the process continues to a second incrementation step 422, where the index i is incremented, and the process returns to step 402. When additional full targets are not required, the target calibration functions ΔCAL,x1 acquired from the included full targets FTi are averaged to give a global target calibration function ΔCAL,GLOBAL. This function is used for calibrating the x-overlay error measurements for all of the half-targets on the semiconductor substrate that are identical to the one included in the calibration process.
As explained above in reference to
Moving substrate 12 with table 20 from measurement site to measurement site, in order to bring each half-target in its turn into the FOV of objective lens 22, may introduce site-to-site variations in the angular misalignment. An angular misalignment aj may be measured for each half-target HT: either by a yaw measurement for each overlay error measurement site or by suitable processing of the captured target image. For example, controller 18 may define two suitably positioned ROIs on the same grating of a half-target, measure the shift between the two projections of the grating bars from the two ROIs, and compute the angular misalignment by dividing the shift by the center-to-center distance between the ROIs. Index i is used here to enumerate the measured half-targets.
When a target calibration function has been determined using full targets, as has been described hereinabove (
Alternatively, in the absence of such a target calibration function, the measured angular misalignment αi may be applied directly as a local correction ΔLOCALi=αi×D. Further alternatively, the angular misalignment αi may be compensated for by an appropriate rotation of table 20 or sensor 28, or a rotation of the captured target image by controller 18.
It will be appreciated that the embodiments described above are cited by way of example, and that the present invention is not limited to what has been particularly shown and described hereinabove. Rather, the scope of the present invention includes both combinations and subcombinations of the various features described hereinabove, as well as variations and modifications thereof which would occur to persons skilled in the art upon reading the foregoing description and which are not disclosed in the prior art.
This application claims benefit of U.S. the Provisional Patent Application 63/299, 010, filed Jan. 13, 2022, which is incorporated herein by reference.
Filing Document | Filing Date | Country | Kind |
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PCT/US22/18812 | 3/4/2022 | WO |
Number | Date | Country | |
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63299010 | Jan 2022 | US |