Abstract:
A method for measuring overlay in semiconductor wafers includes obtaining diffraction based and imaging based measurements of the same target. The two separate measurements are then combined in a way that is consistent to both measurements to obtain an overlay measurement that has high precision and large range.

Description:
PRIORITY CLAIM  
       [0001]    The present application claims priority to U.S. Provisional Patent Application Serial No. 60/426,156, filed Nov. 14, 2002, which is incorporated in this document by reference. 
     
    
     
       TECHNICAL FIELD  
         [0002]    This invention relates to measuring the pattern overlay alignment accuracy of a pair of patterned layers on a semiconductor wafer, possibly separated by one or more layers, made by two or more lithography steps during the manufacture of semiconductor devices.  
         BACKGROUND OF THE INVENTION  
         [0003]    Manufacturing semiconductor devices involves depositing and patterning several overlaying layers. A typical semiconductor wafer might include, for example, a series of gates formed on a first layer and a series of interconnects formed on a second layer. The two layers (and their structures) are formed at different lithography steps in the manufacturing process. Alignment between the two layers is critical to ensure proper connection between the gates and their interconnects. Typically, this means that the tolerance of alignment must be less than the width of a single gate.  
           [0004]    Overlay is defined as the displacement of a patterned layer from its ideal position aligned to a layer patterned earlier on the same wafer. Overlay is a two dimensional vector (Δx, Δy) in the plane of the wafer. Overlay is a vector field, i.e., the value of the vector depends on the position on the wafer. Perfect overlay and zero-overlay are used synonymously. Overlay and overlay error are used synonymously. Depending on the context, overlay may signify a vector or one of the components of the vector.  
           [0005]    Overlay metrology provides the information that is necessary to correct the alignment of the stepper-scanner and thereby minimize overlay error with respect to previously patterned layers. Overlay errors, detected on a wafer after exposing and developing the photoresist, can be corrected by removing the photoresist, repeating exposure on a corrected stepper-scanner, and repeating the development of the photoresist. If the measured error is acceptable but measurable, parameters of the lithography process could be adjusted based on the overlay metrology to avoid excursions for subsequent wafers.  
           [0006]    Most prior overlay metrology methods use built-in test patterns etched or otherwise formed into or on the various layers during the same plurality of lithography steps that form the patterns for circuit elements on the wafer. One typical pattern, called “box-in-box” consists of two concentric squares, formed on a lower and an upper layer, respectively. “Bar-in-bar” is a similar pattern with just the edges of the “boxes” demarcated, and broken into disjoint line segments. The outer bars are associated with one layer and the inner bars with another. Typically one is the upper pattern and the other is the lower pattern, e.g., outer bars on a lower layer, and inner bars on the top. However, with advanced processes the topographies are complex and not truly planar so the designations “upper” and “lower” are ambiguous. Typically they correspond to earlier and later in the process. The squares or bars are formed by lithographic and other processes used to make planar structures, e.g., chemical-mechanical planarization (CMP).  
           [0007]    In one form of the prior art, a high performance microscope imaging system combined with image processing software estimates overlay error for the two layers. The image processing software uses the intensity of light at a multitude of pixels. Obtaining the overlay error accurately requires a high quality imaging system and means of focusing the system. One requirement for the optical system is very stable positioning of the optical system with respect to the sample. Relative vibrations blur the image and degrade the performance. Reducing vibration is a difficult requirement to meet for overlay metrology systems that are integrated into a process tool, like a lithography track.  
           [0008]    As disclosed in U.S. patent application Ser. No. 2002/0158193; U.S. patent application Ser. No. 2003/0190793 A1; and as described in Proc. of SPIE Vol. 5038 February 2003 “Scatterometry-Based Overlay Metrology” by Huang et al., p. 126-137 and “A novel diffraction based spectroscopic method for overlay metrology” by Yang et al. p. 200-207 (all four incorporated in this document by reference) one approach to overcome these difficulties is to use overlay metrology targets that are made of a stack of two diffraction gratings as shown in FIG. 1. The grating stack  10  has one grating  20  in the lower layer and another grating  30  in the upper layer as shown in FIG. 1. The layers of  20  and  30  are to be aligned. There are two instances of the grating stack  10 , one for the x-component of overlay and one for the y-component. The measurement instrument is such that it does not resolve individual grating lines. It measures overall optical properties of the entire grating. Optical properties are measured as a function of wavelength, polar or azimuthal angle of incidence, polarization states of the illumination and the detected light, or any combination of these independent variables. An alternative embodiment uses two stacks of line gratings to measure x-overlay and two stacks of line gratings to measure y-overlay (four grating stacks total). Still another embodiment uses three line grating stacks in combination to simultaneously measure both x and y alignment. (See also PCT publication WO 02/25723A2, incorporated herein by reference). Scatterometry (diffraction) is proving to be an effective tool for measuring overlay.  
           [0009]    A shortcoming of the prior scatterometry-based art is that, diffraction gratings cannot distinguish overlay values that differ by an integer number of periods. Let R(λ,θ,ξ) denote the specular (0-th order) reflection of the grating at wavelength λ, angle of incidence θ, and offset ξ. The offset ξ is the distance between centerlines of lower and upper grating lines as shown in FIG. 1. The function R(λ,θ,ξ) is periodic with respect to the offset ξ: 
             R (λ,θ,ξ)= R (λ,θ,ξ+ P )  (1) 
           [0010]    where P is the period of the grating. The scatterometry-based overlay measurements are even more ambiguous when the profiles of the grating lines are symmetric. Then, a consequence of reciprocity is: 
             R (λ,θ,ξ)= R (λ,θ,−ξ)  (2) 
             R (λ,θ, ( P/ 2)+ξ)= R (λ,θ, ( P/ 2)−ξ)  (3) 
           [0011]    There are two values of offset, separated by P/2, where the optical properties become ambiguous. Optical properties are insensitive to overlay at these points. Therefore, the largest measurement range is P/2 when the grating lines have symmetric cross-sections. If the unit cell of the grating is substantially asymmetric, the measurement range becomes P, a whole period. Huang et al., cited above, describe means of manufacturing a grating with an asymmetric unit cell. The measurement range also becomes a whole period if two grating stacks are used, the offset of each stack is biased, and the two offset biases differ by P/4 (as described in U.S. application Ser. No. 10/613,378, filed Jul. 3, 2003, incorporated in this document by reference).  
           [0012]    [0012]FIG. 2 shows the calculated near-normal incidence, unpolarized reflectance of a grating stack as a function of offset ξ. Each curve corresponds to a different wavelength. The ambiguity described by Equations (2) and (3) is clearly visible in FIG. 2. The ordinate of the graph in FIG. 3 shows overlay measured using diffraction gratings with a 1 μm period and 1:1 line to space ratio. Overlay was obtained by fitting the reflection spectra of a pair of gratings with rigorous coupled wave analysis. The abscissa shows the best estimate of the actual value of overlay, which is the sum of the overlay that was intentionally written to the reticle that produced the gratings and the overlay that was imparted by the lithography stepper-scanner. Overlay measured using gratings is not valid when it approaches or exceeds ±P/4 (250 nm in this example). FIG. 4 is an abstraction that shows the periodic nature of the overlay measured using diffraction gratings. The overlay measured by the grating, Δx GRATING , is related to the actual overlay as follows:  
                   N   =     int        [       Δ                   x   ACTUAL         P   /   2       ]                     Δ                   x   GRATING       =         (     -   1     )     N          [       Δ                   x   ACTUAL       -     N                   P   /   2         ]                     (   4   )                               
 
           [0013]    In Equation (4), int[x] denotes the integer nearest to x. In prior art, the integer N is unknown. Therefore, Δx GRATING  represents Δx ACTUAL  only when N is zero, that is, when |Δx ACTUAL |&lt;P/4. Δx GRATING , which is also called fine-overlay measurement, has high precision but it is only accurate when N=0. Gross overlay is defined as the condition |Δx ACTUAL |&gt;P/4 or |Δy ACTUAL |&gt;P/4, that is, any one component of overlay exceeding a quarter of the period. Gratings cannot detect gross overlay until overlay gets so large that the upper and lower gratings do not overlap in part of the measurement spot. Although gross overlay is rare in well-tuned lithography processes, alignment errors larger than 100 nm, even as large as several microns occur when a new process, a new reticle, or a new projector is introduced. In these instances, there is a need to not only detect but also to measure gross overlay.  
           [0014]    Although increasing the period increases the measurement range, P/2, this approach is not preferred because it reduces the sensitivity of the optical response of grating stacks to overlay. As the period is increased, if the period becomes a significant fraction of the diameter of the measurement spot, the placement of the spot on the grating affects the overlay measurement and reduces its precision. For these two reasons, increasing the period to increase the measurement range is counter-productive. Using more than one grating stack, each with a different period, reduces but does not eliminate ambiguity.  
         SUMMARY  
         [0015]    An embodiment of the present invention provides a method and apparatus for measuring overlay. For a typical implementation, one or more grating stacks are included in a semiconductor wafer. Each grating stack includes an upper grating and a lower grating, each formed on one of the two layers for which overlay is to be measured. Each grating typically has a square or rectangular shape in the X-Y plane defined by the surface of the semiconductor wafer. At least one of the gratings stacks is configured so that its upper grating is larger or smaller (in the X or Y direction) than its lower grating.  
           [0016]    For the method of the present invention, gross overlay is first measured by analyzing one or more grating stacks. Each gross overlay measurement is obtained by measuring, using optical microscopy, a grating stack that includes upper and lower gratings of different size. A fine (i.e., non-gross) overlay measurement is then obtained by scatterometry. Typically, this means that a probe beam is directed at one or more of the grating stacks and the resulting diffraction is analyzed to determine the fine overlay between the upper and lower layers being analyzed.  
           [0017]    The gross and fine overlay measurements are then combined in a way that is consistent with each measurement. Typically, this means that the gross overlay measurement is normalized to locate a starting point for the fine overlay measurement. The fine overlay measurement is then added or subtracted to that starting point to define a total overlay measurement. 
       
    
    
     BRIEF DESCRIPTION OF THE DRAWINGS  
       [0018]    [0018]FIG. 1 shows in cross-section the stack of two gratings that are used in the diffraction-based overlay metrology in the prior art.  
         [0019]    [0019]FIG. 2 shows calculated near-normal specular reflectance of the grating stack in FIG. 1 as a function of offset ξ for four different wavelengths.  
         [0020]    [0020]FIG. 3 shows the overlay measured using grating stacks as shown in FIG. 2 according to the prior art.  
         [0021]    [0021]FIG. 4 is a graph that simplifies and illustrates the periodic nature of the graph in FIG. 3.  
         [0022]    [0022]FIG. 5 shows overlay metrology target according to an embodiment of the present invention.  
         [0023]    [0023]FIG. 6 shows another embodiment for the overlay metrology target configured, in this case to measure overlay in two directions using a single grating stack.  
         [0024]    [0024]FIG. 7 shows another embodiment for the overlay metrology target configured, in this case using 2-dimensional arrays of three-dimensional features such as contact holes, posts, islands.  
         [0025]    [0025]FIG. 8 shows another embodiment for the overlay metrology target configured, in this case to measure overlay in two directions using a single grating stack with each layer in the grating stack being the same size.  
         [0026]    [0026]FIG. 9 shows a schematic diagram of a measurement instrument.  
         [0027]    [0027]FIG. 10 shows the measurement uncertainties for three embodiments of the present invention as a function of actual overlay. 
     
    
     DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS  
       [0028]    Referring to FIG. 5, overlay target  110  contains at least one grating stack  110   x  that measures the x-component of the overlay and at least one grating stack  110   y  that measures the y-component of the overlay. The grating stack  110   x  and  110   y  are, for example, placed in the scribe lines, or alleys, between dies on a semiconductor wafer. Grating stack  110   x  and  110   y  are measured preferably one at a time (sequentially) by an optical instrument. The measurement spot of the optical instrument is  140   x  when it measures grating stack  110   x . The measurement spot then moves to  140   y  to measure grating stack  110   y . Alternatively, the measurement instrument has two measurement spots  140   x  and  140   y  that perform spatially separated but simultaneous measurements. Grating stack  110   x  has a lower grating  120   x  and an upper grating  130   x . Gratings  120   x  and  130   x  differ at least in one dimension. In FIG. 5, the upper grating  130   x  is shown to be shorter than grating  120   x  in the direction of the grating lines. The dimensions of the gratings are such that, both gratings  120   x  and  130   x  completely cover the measurement spot  140   x . The same apply to grating stack  110   y , lower grating  120   y , upper grating  130   y , and measurement spot  140   y . The distances x 1 , x 2 , y 1 , and y 2  shown in FIG. 5 are the widths of the strips where only one of the gratings is visible looking down on the wafer. The x-component of the gross overlay is obtained as ΔX=(x 1 -x 2 )/2. Process induced errors that affect the distances x 1 and x 2  in the same manner are canceled by the differencing operation. In the alternative embodiment shown in FIG. 6, the lower and upper gratings differ in both dimensions. The distances x 1 , x 2 , y 1 , and y 2  are measured on the image of one or more grating stacks.  
         [0029]    [0029]FIG. 7 shows an alternative embodiment where the lower and upper gratings are 2-dimensional arrays of features such as contact holes, posts, islands or other 3-dimensional features. The distances x 1 , x 2 , y 1 , and y 2  are measured on the image of one or more grating stacks. FIG. 8 shows an alternative embodiment where the upper  130   x  and lower  120   x  gratings have the same dimensions. The lower and upper gratings are preferably printed with an offset bias that is large enough to be measured by the imaging system. The overlay is obtained as ΔX=(x 1 +x 2 )/2−(offset bias). This embodiment is not preferred because gross overlay is not obtained from the difference of two similar distances.  
         [0030]    A vision system  200 , such as the one shown in FIG. 9, is used to navigate and find the metrology targets on the wafer  180  and also to measure the distances x 1 , x 2 , y 1 , and y 2 . The vision system consists of a light source  220 , condenser or illumination optics  230 , beam splitter  240 , objective  250 , tube-lens  260 , camera  270  with a CCD or CMOS array detector, image processor  280 .  
         [0031]    In the preferred implementation, the vision system  220  is separate from the system that measures the optical properties of the grating as a function of wavelength or angle of incidence or both. For example, FIG. 9 shows an oblique incidence ellipsometer  300  that measures the optical properties of the gratings. The components of ellipsometer  300  are broadband light source  310 , collimator  320 , rotary polarizer  330 , optional rotary waveplate  340 , refractive or reflective illumination objective  350 , collection objective  360 , optional rotary waveplate  370 , rotary polarizer  380 , re-imaging optics  390 , pinhole  392 , grating spectrometer  394 . Optical components  230 ,  250 ,  260 ,  320 ,  350 ,  360 , and  390  can be compound refractive or reflective lenses. A normal or oblique incidence, polarized or unpolarized reflectometer can also be used to measure the optical properties of the grating stacks. The spectroscopic metrology system can also share its optical path with the vision system (not shown in FIG. 9).  
         [0032]    The vision system measures the distances x 1 , x 2 , y 1 , y 2 , and some known and well-controlled distance G x , and G y  to calibrate the pixels in micrometers. In the simplest example, G x , and G y  can be the x and y dimensions of a grating as shown in FIG. 5. This embodiment is not preferred because line end shortening would affect G y . In a more preferred embodiment, the calibration distances G x , and G y  are distances between identical features. The following differences are formed from the measurements of the vision system: 
         Δ X   VISION =( x   1   -x   2 )/2  (5) 
         Δ Y   VISION =( y   1   -y   2 )/2  (6) 
         [0033]    This is similar to the box-in-box measurements in imaging-based prior art except the boxes are not stacks of thin films but stacks of gratings. The overlay measurement (ΔX VISION , ΔY VISION ), which is a measurement of gross overlay, is less precise than grating measurements but it has a significantly larger measurement range. The range of the overlay measurement by the vision system is equal to the distance from the grating stack to the edge of the field of view of the camera or the distance from the grating stack to the nearest structure on the wafer, whichever distance is smaller. Typically, this range is at least 2 micrometers.  
         [0034]    Embodiment-1 for Combining Image and Diffraction-Based Overlay Measurements  
         [0035]    In one embodiment of the invention, overlay is measured as:  
               Δ                   x   MEAS       =     {             Δ                   x   GRATING                                  if                               |     Δ                   x   VISION       |     &lt;     P   4                     Δ                   x   VISION                   if                |     Δ                   x   VISION       |     ≥     P   4                         (   7   )                               
 
         [0036]    The total measurement uncertainty of the vision-based overlay measurement, TMU VISION , is preferably no greater than P/8. The y-component of overlay is calculated in an analogous fashion. In this embodiment, the measurement uncertainty is determined by the diffraction-based measurement when |Δx ACTUAL |&lt;P/4−TMU VISION . The measurement uncertainty is determined by the vision system when |Δx ACTUAL |&gt;P/4+TMU VISION . Curve  400  in FIG. 10 shows a Monte-Carlo simulation of the measurement uncertainty for this embodiment. In this simulation, the measurement uncertainties of the vision and grating systems are ±P/8 and ±P/1000 respectively. Random measurement errors were uniformly distributed in a ±P/8 neighborhood for the vision-based measurement and a ±P/1000 neighborhood for the diffraction-based measurement.  
         [0037]    Embodiment-2 for Combining Image and Diffraction-Based Overlay Measurements  
         [0038]    In another embodiment of the invention, the vision and diffraction-based overlay measurements are combined as follows:  
                   M   =     int        [       Δ                   x   VISION         P   /   2       ]                     Δ                   x   MEAS       =           (     -   1     )     M        Δ                   x   GRATING       +     M                   P   /   2                       (   8   )                               
 
         [0039]    M is an estimate of the integer N in Equation (4). The estimate is obtained from the vision-based overlay measurement. Given that overlay is in M th  half-period, a high-precision Δx MEAS  is obtained from the diffraction-based measurement as described by the second equation in (8). The y-component of overlay is obtained in an analogous fashion. In this embodiment, the precision of overlay is determined by the diffraction-based measurement except at the dead-points of the diffraction-based measurement where the diffraction based-measurement is not sensitive to overlay. For a single grating stack with an offset bias of P/4, or for two grating stacks with offset biases of +P/4 and −P/4, sensitivity to overlay diminishes when overlay is an odd multiple of P/4 as seen in FIGS. 3 and 4. In this case, Δx MEAS  according to Equation (8) has the precision of the diffraction based measurement for all overlay values except the ones close to odd multiples of P/4. When overlay is in a TMU VISION  wide neighborhood of an odd multiple of P/4, the precision of Δx MEAS  is equal to that of ΔX VISION . TMU VISION  is required to be no larger than P/8 in this embodiment. The measurement uncertainty for this embodiment is shown by curve  410  in FIG. 10.  
         [0040]    Embodiment-3 for Combining Image and Diffraction-Based Overlay Measurements  
         [0041]    In this embodiment, at least two grating stacks are used to measure overlay in one direction. The two gratings differ in offset bias by P/4. They yield the following diffraction-based overlay measurements, not accounting for measurement errors:  
                     N   1     =     int        [       Δ                   x   ACTUAL         P   /   2       ]                     Δ                   x     GRATING   -   1         =         (     -   1     )       N   1            [       Δ                   x   ACTUAL       -       N   1                     P   /   2         ]                     N   2     =     int        [         Δ                   x   ACTUAL       +     (     P   /   4     )         P   /   2       ]                     Δ                   x     GRATING   -   2         =         (     -   1     )       N   2            [       Δ                   x   ACTUAL       +     (     P   /   4     )     -       N   2                     P   /   2         ]                     (   8   )                               
 
         [0042]    The overlay measurements are combined as follows:  
                     M   1     =     int        [       Δ                     x                VISION         P   /   2       ]                     M   2     =     int        [         Δ                   x   VISION       +     (     P   /   4     )         P   /   2       ]                     Δ                   x   MEAS       =     {               Δ                       x     GRATING   -   1            (     -   1     )         M   1         +         M   1          (     P   /   2     )                     if       |     Δ                   x     GRATING   -   1         |     &lt;     P   /   8                       Δ                       x     GRATING   -   2            (     -   1     )         M   2         +       M   2          (     P   /   2     )       -       (     P   /   4     )                   if                  |     Δ                   x     GRATING   -   1         |     ≥     P   /   8                               (   9   )                               
 
         [0043]    Provided that TMU VISION  is no greater than P/8, the precision of Δx MEAS  is equal to the precision of the diffraction-based overlay even for gross overlay. The measurement uncertainty for this embodiment is shown by curve  420  in FIG. 10.