PATENT ABSTRACT
Photoresist on a wafer is exposed using tiles on a mask that improve flare performance. Features that are not to be exposed on the photoresist correspond to features on the mask. The various features are surrounded by other features that vary and thus affect flare differently. Selected features have tiles added nearby but also far enough away to improve uniformity in the effects of flare on the various features that are intended to be present in the photoresist. The tiles are made either very small in width or partially absorbing so that the tiles are not resolved in the photoresist. Thus the tiles reduce flare but do not alter the desired pattern in the photoresist.

PATENT DESCRIPTION
CROSS REFERENCE TO RELATED APPLICATION  
       [0001]    This application is related to:  
         [0002]    U.S. patent application Ser. No. 09/873,810, entitled “Method of Forming An Integrated Circuit Device Using Dummy Features and Structure Thereof,” filed Jun. 4, 2001, and assigned to the assignee hereof. 
     
    
     
       FIELD OF THE INVENTION  
         [0003]    This invention relates generally to semiconductor circuits, and more specifically, to the manufacture of semiconductors.  
         BACKGROUND OF THE INVENTION  
         [0004]    Integrated circuit manufacturing uses photolithography to transfer patterns from a master mask to a semiconductor substrate. As feature dimensions used in integrated circuits have become sub-micron various problems are encountered. The small dimensions approach the physical capability of photolithography. At such dimensions, the nonplanarity of surfaces, such as wafers have a significant affect on feature resolution on the wafer. A known compensation technique is the use of tiles which are additional features formed on the semiconductor substrate in areas that are not used for functional circuitry. Tiling is used to improve the planarity or flatness of the substrate surface after a conventional chemical/mechanical polish (CMP) step. Tiling can also be used to equalize the chemical concentration during an etch step and ensure that the concentration is uniform across a wafer. A major limitation with tiling is that tiling cannot be used in close proximity to functional circuitry because of negative effects on device characteristics.  
           [0005]    Another known compensation technique to compensate light diffraction at submicron dimensions is referred to generally as sub-resolution features or scattering bars. This technique involves the placement of small features on the mask in close proximity to the small isolated desired design features. The scattering bars are placed within less than three times the minimum feature spacing. Scattering bars make isolated features pattern as if they are dense features in that they decrease the sensitivity to focus variations in a photolithographic system. Another known lithography problem is referred to as flare which is the existence of scattered background light in a lithographic system. Flare is dependent upon the pattern density of a mask. As flare varies, there is also variation in wafer feature dimensions. Scattering bars may offer some improvement in highly local flare reduction and pattern uniformity. However the scattering bars do not provide improvement for medium or long range pattern density or flare distortion.  
           [0006]    Another known lithographic issue is the variation of mask or reticle feature dimensions as mask pattern density varies. Tiling offers some improvement to this issue but tiling is limited in use due to the electrical modifications on functional devices as mentioned above. Subresolution scattering bars do not offer significant improvement to this problem. For both flare and reticle feature dimensions, there are solutions known as biasing feature edges. These solutions are generally referred to as optical proximity correction (OPC). A problem with these solutions is that they require extremely intense computation for every feature edge as to what is the impact of flare or reticle pattern density. 
       
    
    
     BRIEF DESCRIPTION OF THE DRAWINGS  
       [0007]    The present invention is illustrated by way of example and is not limited by the accompanying figures, in which like references indicate similar elements.  
         [0008]    [0008]FIG. 1 illustrates in perspective form a semiconductor lithography system with a reflective mask, such as an extreme ultraviolet (EUV) system;  
         [0009]    [0009]FIG. 2 illustrates in perspective form a semiconductor lithography system with a transmitting mask, such as a deep ultraviolet (DUV) system;  
         [0010]    [0010]FIG. 3 illustrates a top view of a portion of a reflecting mask pattern transferred to a wafer with flare error;  
         [0011]    [0011]FIG. 4 illustrates a top view of a portion of a reflecting mask pattern transferred to a wafer with reduced but undesired flare error;  
         [0012]    [0012]FIG. 5 illustrates a top view of a portion of a reflecting mask pattern transferred to a wafer with reduced flare error in accordance with one form of the present invention;  
         [0013]    [0013]FIG. 6 illustrates a top view of a reflecting mask pattern transferred to a wafer with reduced flare error in accordance with another form of the present invention;  
         [0014]    [0014]FIG. 7 illustrates a perspective view of an integrated circuit pattern on a mask incorporating the previously discussed pattern portions;  
         [0015]    [0015]FIG. 8 illustrates a perspective view of a reflecting mask having a plurality of integrated circuits and having flare compensation inside and beyond the reflecting mask; and  
         [0016]    [0016]FIG. 9 illustrates in cross-section form a reflecting mask with flare compensation. 
     
    
       [0017]    Skilled artisans appreciate that elements in the figures are illustrated for simplicity and clarity and have not necessarily been drawn to scale. For example, the dimensions of some of the elements in the figures may be exaggerated relative to other elements to help improve the understanding of the embodiments of the present invention.  
       DETAILED DESCRIPTION  
       [0018]    [0018]FIG. 1 illustrates an EUV lithography system or optical system  10  with an optical portion  11 . Optical system  10  has a radiation source  12 , a reflecting reticle or reflecting mask  18 , and optical reflecting elements  20 ,  22 ,  24 ,  26  and  28 . In one form, the optical reflecting elements  20 ,  22 ,  24 ,  26  and  28  are implemented with multiple layer mirrors. The radiation source  12  may be implemented in various forms such as a laser, a laser produced plasma, a gas discharge source or an electron beam source. In the illustrated form, light produced by the radiation source  12  is transferred from the radiation source  12  to the reflecting mask  18 . A predetermined pattern exists on the reflecting mask  18 . Portions of the predetermined pattern cause the radiation or light to reflect via the reflective mask by reflecting from reflecting mask  18  to an optical reflecting element  20 . In sequential fashion the light is further reflected to optical reflecting elements  22 ,  24 ,  26  and  28 . From optical reflecting element  28  the light is reflected to a photoresist layer in the form of photoresist  16  on a surface of a wafer  14  for the formation of a semiconductor device. Where light contacts photoresist  16 , the photoresist  16  is rendered soluble by subsequent processing steps involving heating.  
         [0019]    Unfortunately the optical system  10  is subject to non-specular reflection caused by roughness of the surfaces of reflecting mask  18  and each of the optical reflecting elements  20 ,  22 ,  24 ,  26  and  28 . Roughness in the reflecting mask translate into focal errors at the wafer  14 . Roughness in the optical reflecting elements  20 ,  22 ,  24 ,  26  and  28  translate into flare on wafer  14  that distorts the pattern intended to be transferred to wafer  14 .  
         [0020]    Illustrated in FIG. 2 is a DUV (deep ultraviolet) system or optical system  50  generally having a radiation source  52 , a transmission mask or a transmitting mask  56 , projection optics  54  and a semiconductor wafer  58  having overlying photoresist  60 . Transmitting mask  56  is an optically transmissive mask and has both transmissive portions and absorbing portions. The radiation source  52  is implemented with either a laser or a gas discharge source. Light from radiation source  52  is transferred to the transmitting mask  56  that has a predetermined mask pattern thereon. The light transfers through the transmissive portions of the transmitting mask  56  and is directed via projection optics  54  onto the photoresist  60 . Projection optics  54  may be implemented with a combination of refractive lenses and mirrors. The photoresist  60  is rendered soluble in those areas where light contacts the photoresist  60  by subsequent heating. There are numerous error sources in transferring the patterning from transmitting mask  56  to wafer  58  including roughness on the optical surfaces of the projection optics  54 , inhomogeneities associated with the lens materials and undesired light reflections.  
         [0021]    Illustrated in FIG. 3 is a top view of a portion of a reflecting mask pattern transferred to a wafer with flare error. A flare proximity region  70  of a mask, such as reflecting mask  18  of FIG. 1, contains a pattern that is desired to be printed onto wafer  14 . The flare proximity regions described herein may extend for several millimeters and include multiple sub-regions of varying pattern density. Flare effects are therefore imaging effects over both short and long ranges. It should be understood that transmitting mask  56  of FIG. 2 is analogous. Only a small portion of a complete pattern is illustrated for ease of explanation. It should be noted that the desired features have well defined edges such as a straight-edge and square corners. Due to the errors described above in connection with either optical system  10  or optical system  50 , the resulting pattern on a wafer, such as wafer  14  of FIG. 1, is significantly distorted within a flare proximity region  72 . The wafer features are smaller and are not well defined. Such feature distortions typically are unacceptable as the modified features change the electrical characteristics and functionality of the associated circuitry. It should be noted that for illustration purposes only that within each of flare proximity region  70  and flare proximity region  72  there is no other feature than the desired feature to be patterned.  
         [0022]    Illustrated in FIG. 4 is a top view of a portion of a reflecting mask pattern transferred to a wafer with reduced but undesired flare error. A section of mask  18  contains multiple features within a flare proximity region  74  and an analogous section of wafer  14  contains the same multiple features within a flare proximity region  76 . Assume for explanation purposes that flare proximity region  74  is comparable to flare proximity region  70  and that flare proximity region  76  is comparable to flare proximity region  72 . The flare error is reduced by the presence of other features within the flare proximity region  74 . There are three features within the section of mask  18  that are analogous to that illustrated in FIG. 3. Additionally, there are four additional features within flare proximity region  74  that were not included within flare proximity region  70 . Therefore, it should be noted that the increased pattern density significantly reduces the distortion from flare in the transferred pattern. What this phenomena means is that there can be large variation over a single integrated circuit pattern in flare based upon the pattern density.  
         [0023]    Illustrated in FIG. 5 is a top view of a portion of a reflecting mask pattern transferred to a wafer with reduced flare error. A flare proximity region  78  of mask  18  generally has a plurality of features desired to be transferred and one or more tiles having a length and a width such as tiles  82 ,  84 ,  86   88 ,  90  and  92 . The length of the tiles is longer than a length of a correlated pattern feature by at least one hundred percent (100%). The tiles  82 ,  84 ,  86 ,  88 ,  90  and  92  do not get transferred onto the target wafer  14  having a flare proximity region  80 . The reflecting mask has an absorbing portion made up of the feature patterns (not numbered) that reflect a portion of incident radiation while largely being absorbing. The tiles  82 ,  84 ,  86 ,  88 ,  90  and  92  reduce the pattern distortion from flare for a flare proximity region that does not have high pattern density. In order to keep each of tiles  82 ,  84 ,  86 ,  88 ,  90  and  92  from appearing on the target wafer  14 , the width of each of tiles  82 ,  84 ,  86 ,  88 ,  90  and  92  is less than 0.3 multiplied by the magnification factor, and the wavelength of the radiation source, divided by the numerical aperture of the optical system  10  or  54 . The magnification factor is the size of the features on the mask  18  divided by the size of the features on the wafer  14 . The numerical aperture of the optical system  10  or  54  is the sine of the angle subtended by the exit pupil of the optical system at the plane of wafer  14 . In addition to the width of each of tiles  82 ,  84 ,  86 ,  88 ,  90  and  92  being important, the placement of these tiles is also important. The features within flare proximity region  78  that are to be transferred onto wafer  14  must be separated from each other by a predetermined minimum spacing. Tiles  82 ,  84 ,  86 ,  88 ,  90  and  92  should therefore be positioned relative to the transferred features at a minimum distance from the transferred features that is approximately four times or greater than the minimum spacing. While not all tiles necessarily have a minimum distance of four times or greater the minimum spacing, the majority of the tiles do, if not all. Tiles  82 ,  84 ,  86 ,  88 ,  90  and  92  are fully radiation absorbing and help significantly to reduce undesired reflected light.  
         [0024]    In addition to the tiles  82 ,  84 ,  86 ,  88 ,  90  and  92 , additional tiles in the form of diffraction bars  81 ,  83 ,  85 ,  87 ,  89 ,  91  and  93  may optionally be positioned in very close proximity to the pattern features to be transferred to wafer  14 . Diffraction bars  81 ,  83 ,  85 ,  87 ,  89 ,  91  and  93  are closer to the pattern features than anywhere from 0.8 to three times the minimum spacing between the transferred pattern features. Diffraction bars  81 ,  83 ,  85 ,  87 ,  89 ,  91  and  93  function to provide sub-resolution assistance by changing the diffraction pattern of an isolated pattern feature to look like the diffraction pattern of a set of densely clustered pattern features. Therefore, while good pattern feature fidelity is provided by the use of tiles  82 ,  84 ,  86 ,  88 ,  90  and  92 , even better pattern fidelity is provided when diffraction bars  81 ,  83 ,  85 ,  87 ,  89 ,  91  and  93  are also used.  
         [0025]    The use of tiles  82 ,  84 ,  86 ,  88 ,  90  and  92  also improves the control of the mask critical dimensions (CDs) due to reductions in mask manufacturing proximity effects. In general, the mask manufacturing proximity effects have a similar proximity range as the flare proximity range and are therefore correctable by the same tiles  82 ,  84 ,  86 ,  88 ,  90  and  92 . These improvements in mask CD control create an improvement in control of the wafer feature CDs and therefore improve circuit electrical performance.  
         [0026]    Illustrated in FIG. 6 is a top view of a reflecting mask pattern transferred to a wafer with reduced flare error. A flare proximity region  94  within mask  18  has the three previously illustrated features that are transferred to wafer  14  within a flare proximity region  96 . Additionally, tiles  98 ,  100  and  102  are positioned around the features. Tiles  98 ,  100  and  102  have a significantly greater width and area than the tiles  82 ,  84 ,  86 ,  88 ,  90  and  92  of FIG. 5. Also, some of tiles  98 ,  100  and  102  have an area that is larger than some or all of the pattern features of flare proximity region  94 . The tiles  98 ,  100  and  102  are not fully absorbing, but rather are partially attenuating or partially absorbing. Tiles  98 ,  100  and  102  absorb at least an additional 20% of the radiation incident on the tiles to that absorbed by the reflecting portion of pattern features of the mask. It should be noted that for additional fidelity, diffraction bars such as diffraction bars  81 ,  83 ,  85 ,  87 ,  89 ,  91  and  93  of FIG. 5 may also be used in the embodiment of FIG. 6. Tiles  98 ,  100  and  102  are to be positioned with respect to the transferred features and within flare proximity region  94  using the same rules for spacing as described above for tiles  82 ,  84 ,  86 ,  88 ,  90  and  92 . Tiles  98 ,  100  and  102  also reduce undesired reflection with their partial radiation absorbing characteristic. By making the tiles  98 ,  100  and  102  only partially radiation absorbing, we have discovered that the tiles  98 ,  100  and  102  do not print onto or get transferred to the wafer  14 . Therefore, the tiles  98 ,  100  and  102  may be made physically much larger than previous tiles that would transfer since such tiles were fully absorbing.  
         [0027]    The use of tiles  98 ,  100  and  102  also improves the control of the mask CDs due to reductions in mask manufacturing proximity effects. In general, the mask manufacturing proximity effects have a similar proximity range as the flare proximity range and are therefore correctable by the same tiles  98 ,  100  and  102 . These improvements in mask CD control create an improvement in control of the wafer feature CDs and therefore improve circuit electrical performance.  
         [0028]    Illustrated in FIG. 7 is a perspective view of an integrated circuit pattern  95  on a mask incorporating the previously discussed flare proximity regions  70 ,  78 ,  94  and  74 . Flare variation will differ for each of the flare proximity regions due to differences in the pattern density. Therefore, the pattern fidelity distortion associated with flare differs depending upon what portion of the integrated circuit pattern  95  is being processed.  
         [0029]    Illustrated in FIG. 8 is a perspective view of mask  18  from previous figures in which multiple integrated circuit patterns are grouped together into one mask  18 . This permits the simultaneous production of multiple integrated circuits. In the illustrated form, integrated circuit patterns  110 ,  112 ,  114 ,  116 ,  118  and  120  are implemented in a joined array for a plurality of die. Each of integrated circuit patterns  110 ,  112 ,  114 ,  116 ,  118  and  120  may, in one form, represent the same pattern as integrated circuit pattern  95  of FIG. 7. Peripheral to the integrated circuit patterns  110 ,  112 ,  114 ,  116 ,  118  and  120  is a perimeter region in the form of a radiation absorbing border  122  for absorbing radiation. Since the radiation absorbing border  122  represents an abrupt change in pattern density from the integrated circuit patterns, it is desired to make the radiation absorbing border  122  become partially absorbing. In one form, radiation absorbing border  122  is implemented by chrome. By reducing the thickness of chrome used to implement radiation absorbing border  122 , the amount of absorption of radiation absorbing border  122  can be reduced. This reduction in absorption at the border makes the amount of flare distortion across the integrated circuit pattern more uniform. With a completely absorbing border, the amount of flare at the periphery of the integrated circuit pattern is significantly lower than the amount of flare in the center of the integrated circuit pattern. Therefore, by making the border partially absorbing, the amount of flare at the periphery is increased to more closely match the flare in the central portion of the integrated circuit pattern. Another technique that might be used to make the radiation absorbing border  122  be partially absorbing is to insert one or more sub-resolution slots, such as a slot  123 , in the radiation absorbing border  122  that will not be transferred to a wafer.  
         [0030]    Illustrated in FIG. 9 is a cross-section of reflecting mask  18  with flare compensation. A substrate  150  has an overlying multilayer or multiple layer structure  152  that functions to reflect incoming radiation from a radiation source. Over a portion of the multiple layer structure  152  is an absorber layer in the form of an absorbing film stack  151  that represents but one of a plurality in a pattern of absorbing features on a substrate  150  of reflecting mask  18 . The absorbing film stack  151  may have one or multiple layers. In the illustrated form, an absorbing layer or a first layer  160  and a second layer  158  are used. Typical materials include, for example, silicon dioxide, chrome, tantalum silicon nitride, tantalum nitride and molybdenum silicide. An upper or top portion of the multiple layer structure  152  includes a region  154 . Within region  154  is an area  156  where region  154  is changed to be partially absorbing. There are various percentages in the amount of absorption that may be implemented. Generally, the amount of change in absorption of area  156  is at least twenty percent greater than the other portions of region  154  outside of area  156 . In other words, there is provided a partially reflecting tile that absorbs at least an additional 20% of the radiation incident on the tile to that absorbed by the more reflecting portions of the mask. Typically this percentage will be greater, such as thirty percent or more, but may also be less than twenty percent. There are at least two embodiments to make reflecting mask  18  partially absorbing. Absorbing film stack  151  may be made partially absorbing by thinning, reducing or even removing the thickness of one or more of the multiple layers, such as thinning at least second layer  158 . Another method to make reflecting mask  18  partially absorbing and create a desired reflectance is to convert, modify or ‘damage’ area  156  of region  154  such as by heating or annealing area  156 . In one form, the modifying is accomplished by applying an electron beam to the selected area  156 . Another method is to convert the selected area  156  by applying a laser beam to area  156 . Yet another method is to convert area  156  by applying an ion beam to area  156 .  
         [0031]    By now it should be appreciated that there has been provided methods and a semiconductor optical system that minimizes the reduction in feature fidelity caused by flare. The anti-flare features described herein reduce flare diffraction effects on the order of greater than four times a wavelength of the illumination. The methods taught herein may be used to apply tiling for flare reduction to areas that are not able to accept a standard tile which resolves on the wafer. The partially transmissive/reflective tiles can be large enough in size to be easily patterned on a mask or reticle. Where size is more of a constraint, the tiles may be sized with a maximum width as taught above to reduce flare and also not resolve on the wafer. Because the features used herein for flare compensation are positioned far enough from features that will appear on a wafer, the compensating features do not appreciably change the radiation diffraction associated with the features to be transferred. When the mask is implemented as a reflecting mask having reflecting portions and absorbing portions, each of the tiles provided for anti-flare purposes forms an absorbing portion.  
         [0032]    In the foregoing specification, the invention has been described with reference to specific embodiments. However, one of ordinary skill in the art appreciates that various modifications and changes can be made without departing from the scope of the present invention as set forth in the claims below. For example, the flare compensation method may be used for any value of radiation wavelength. The present invention is not limited to any particular type of semiconductor material or radiation source. Both transmitting and reflective masks and both positive and negative photoresist may be used herein. Various optical systems such as e-beam systems may be implemented. Improvements in critical dimension (CD) feature resolution is realized for short, medium and long range dimensions in a wafer. Accordingly, the specification and figures are to be regarded in an illustrative rather than a restrictive sense, and all such modifications are intended to be included within the scope of the present invention.  
         [0033]    Benefits, other advantages, and solutions to problems have been described above with regard to specific embodiments. However, the benefits, advantages, solutions to problems, and any element(s) that may cause any benefit, advantage, or solution to occur or become more pronounced are not to be construed as a critical, required, or essential feature or element of any or all the claims. As used herein, the terms “comprises,” “comprising,” or any other variation thereof, are intended to cover a non-exclusive inclusion, such that a process, method, article, or apparatus that comprises a list of elements does not include only those elements but may include other elements not expressly listed or inherent to such process, method, article, or apparatus. The terms a or an, as used herein, are defined as one or more than one. The term plurality, as used herein, is defined as two or more than two. The term another, as used herein, is defined as at least a second or more. The terms including and/or having, as used herein, are defined as comprising (i.e., open language). The term coupled, as used herein, is defined as connected, although not necessarily directly, and not necessarily mechanically.