SEM image enhancement using narrow band detection and color...

Radiant energy – Inspection of solids or liquids by charged particles – Electron probe type

Reexamination Certificate

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C250S311000, C250S397000, C250S492200

Reexamination Certificate

active

06201240

ABSTRACT:

FIELD OF THE INVENTION:
The present invention relates to scanning electron microscopes (SEM) and, more particularly, to enhancing images of SEM using narrow band detection and color assignment. The invention is particularly useful in the general field of inspection and review of defects in the semiconductor wafers fabrication process.
BACKGROUND OF THE INVENTION
Scanning electron microscopes (SEM) are very useful for imaging very small elements on a sub-micron scale, with a resolution on the order of nanometers. Therefore, various SEM systems are used in the semiconductor industry for engineering and metrology. Recently, much attention has also been given to the use of SEM in investigation of defects on semiconductor circuits. Since the size of defects of interest (i.e., killer defects) continues to shrink with the shrinking of the design rules, there's a continuous need for improvement in the images obtained by such SEM.
As is well known to those skilled in the art, SEM images are obtained by directing a primary electron beam onto a sample, and using detectors to collect electrons returned from the sample. Some of these electrons are back scattered electrons (BSE) reflected as a result of elastic collisions. Others are secondary electrons (SE) emitted from the sample as a result of inelastic collisions. For better understanding of the discussion that follows, the reader's attention is directed to
FIG. 1
, depicting the energy spectrum of electrons emitted from a sample upon the impingement of a primary electron beam (the plot is adopted from Image Formation in Low-Voltage Scanning Electron Microscopy, L. Reimer, SPIE, Vol. TT12). It is conventionally accepted that collected electrons having energy up to 50 eV are SE, while collected electrons having energy above 50 eV are BSE.
SEM images have been traditionally provided as gray scale. However, for some time there has been an effort to provide color SEM images. Two basic methods have been employed for applying color to SEM images. The first method is based on the fact that the human eye is more sensitive to color variation than to shades of gray. Therefore, the gray scale was used to modulate color and it is sometimes referred to as color modulation. Another method was developed basically to better distinguish between features in two different signals (for example, one of SE and one of BSE). Thus, each signal was color coded and the resulting signals combined to obtain a color picture. The journal SCANNING has dedicated an entire issue to color SEM and much information about these systems is disclosed there—SCANNING, Vol 3, 3, (1980). One article in that issue, COLOR CONVERSION IN ELECTRON MICROSCOPY, by A. V. Crewe, aptly summarizes the advantages of color in SEM and the various techniques used for color SEM images.
As is known in the art, and as can be understood from the above noted works, SEM images are generally created from SE or BSE depending on the purpose of the study. That is, when the study requires the ability to distinguish between different materials in the sample, BSE detectors are used. See, for example, COLOUR ENCODING OF VIDEO SIGNALS IN SEM, E. I. Rau, et al., Id. On the other hand, when it is important to understand the topography of the sample, SE detectors are used. See, for example, U.S. Pat. No. 5,212,383 describing color modulation of wide energy band SE signals. Moreover, by assigning a certain color to a SE detector and another color to a BSE detector and then combing the images, one can obtain material and topography information in the same image. See, for example, A METHOD FOR PREPARING COLORED SCANNING ELECTRON MICROGRAPHS USING SE AND BSE IMAGES, K. Tanaka, Id.
However, in spite of the above efforts, there are still particular deficiencies of SEM images that are not addressed by these systems. These deficiencies are of particular interest to the semiconductor industry. One particular issue of importance to the semiconductor industry is a clear delineation of edges of features. For example, when one takes a SEM image of a bit line, it is important that the edges of the bit line be clearly displayed so that the edges can be investigated. Similarly, when one takes a SEM image of a defect, it is important to clearly distinguish the edges of the defect so that its boundaries can be determined.
Another issue of interest is clear contrast of materials. Specifically, theoretical and experimental works showed the capabilities of using BSE for distinguishing between heavy elements, but BSE lacked this capability for the light elements. Thus, a better method is needed for distinguishing between elements, especially when similar, light, elements are present within the investigated sample.
Voltage Contrast is a common way to test the electrical connectivity of features in the semiconductor industry. In one of the Modes of Voltage Contrast-Passive Voltage Contrast (PVC)—all the conductors that are grounded yield different signal from those that are not grounded. This happens because those conductors that are not grounded and float on the insulator are charged and they usually exhibits higher emission yield. There is a need to be able to enhance and diminish this effect on the resulting image, as needed for particular applications.
SUMMARY OF THE INVENTION
The present invention provides a system and a method for solving the above noted deficiencies of the prior art systems. Specifically, the disclosed invention allows for enhancement of the edges of a feature, enhancement of material contrast, topography contrast and the control of the contrast in the PVC mode of Voltage Contrast SEM images.
According to one feature of the present invention, at least two detectors are used to collect secondary electrons emanating from the sample. The detectors are controlled to collect a specific narrow band of secondary electrons, and the band of one detector is set to be different from the band of the other. Control of the bands of each detector allows for enhancements of various features, such as edge, material, and PVC contrast, in the resulting image. For example, edge contrast is enhanced by adjusting an SE detector to collect electrons of very low energy. On the other hand, topography enhancement is achieved by collecting SE at the higher end of the spectrum.
According to another feature, the various features are enhanced by using various combinations of the images obtained from the different detectors. For example, adding an edge enhanced image (slow electrons) to a topographic enhanced image (fast electrons) provides an image wherein both the topography and edges are enhanced.
Detector location also influences the resulting image. For example, if a secondary detector is placed at a relatively large angle to primary beam, shadow effects can be obtained, much in the same way as if one was to illuminate the feature from the side with a flash light. The bandwidth of such a detector can also be controlled to obtain topography enhancement. Moreover, combining the image of such a detector with edge enhanced and material enhanced images can provide a single image wherein the edges, material, and topography features are enhanced.
Another feature of the disclosed invention resides in color coding the images obtained from the narrow band SE detectors. Specifically, as noted above, combining the images of the various narrow band SE detectors results in an overall enhanced image. However, such an image includes much information that is hard to perceive in a gray scale. Therefore, according to the present invention, various color coding is used to allow the human eye to better appreciate the vast amount of information resulting from the combination of the various images.


REFERENCES:
patent: 3628014 (1971-12-01), Gruble, Jr.
patent: 4041311 (1977-08-01), Martin
patent: 4560872 (1985-12-01), Antonovsky
patent: 4689555 (1987-08-01), Brust et al.
patent: 5212383 (1993-05-01), Scharf
patent: 5644132 (1997-07-01), Litman et al.
patent: 6066849 (2000-05-01), Masnaghetti et al.
“Color Voltage Contrast: A New Method of Implemen

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