Abstract:
The surface of an epitaxial wafer is inspected using an optical scattering method. The intensities of light scattered with a narrow scattering angle and light scattered with a wide scattering angle reflected from laser light scatterers (LLS) on the wafer surface are detected. If the intensifies of narrowly and widely scattered lights are within a prescribed sizing range, it is judged whether the laser light scatterer is a particle or killer defect by deciding into which zone ( 410, 414, 418, 439 ) within the sizing range the PLS size based on the narrowly scattered light intensity and the PLS size based, on the widely scattered light intensity fall. If the intensity of the narrowly or widely scattered light exceeds the sizing range ( 417, 420, 421, 423, 424, 425 ), or if a plenty of laser light scatterers are continuous or concentrated ( 422 ), the laser light scatterers are judged to be killer defects.

Description:
CROSS REFERENCE TO RELATED APPLICATIONS 
   The present application is a continuation of PCT/JP 50/07120, filed on Apr. 13, 2005, and is related to and claims priority from Japanese patent application no. 2005-152672, filed on Apr. 13 2004. The content of both of the aforementioned applications are incorporated herein by reference. 

   TECHNICAL FIELD 
   The present invention relates to technology for inspecting the surface quality of a semiconductor wafer, suitable, in particular, to the detection of surface defects of an epitaxial wafer. 
   BACKGROUND ART 
   In general, semiconductor wafer defects (structural or chemical abnormalities that impair the ideal crystal structure of the surface layer of the semiconductor wafer) are classified in terms of the effect that they have on a semiconductor device that is formed on the wafer into slight defects, which are allowable, and fatal defects. Fatal defects are called “killer defects” and result in a lowering of the yield of semiconductor devices. In particular in the case of epitaxial wafers, the main defects are stacking faults (SF) of the epitaxial layer; usually, these appear as protuberances or concavities of the surface of the semiconductor wafer. Most killer defects are part of such an SF. Killer defects are caused for example by the height being such as to generate a defocusing fault in the process of manufacturing a device, or by a defect termed a large area defect (LAD), having a wide area, that affects several devices. For convenience, defects including surface defects of epitaxial wafers will herein be referred to as ELDs (EP layer defects). Techniques for detecting “killer defects” on the surface of semiconductor wafers are extremely important in semiconductor manufacture. 
   An abnormality inspection device employing an optical scattering method is widely employed for surface inspection of semiconductor wafers. Using such an abnormality inspection device, the surface of a semiconductor wafer is scanned with a laser beam of minute size and scattered light from laser light scatterers (defects or particles) on the surface of the semiconductor wafer is detected; the size (value corresponding to the size of standard particles (PLS; polystyrene latex)) of laser light scatterers present on the wafer surface is measured from the intensity of this scattered light. Whereas it is impossible to permanently remove defects from semiconductor wafers, particles can be removed by subsequent processing and are not therefore fatal as regards the semiconductor device. Consequently, in surface inspection using an optical, scattering method, it is important to be able to distinguish whether the individual laser light scatterers that are detected are defects or particles. 
   Laid-open Japanese Patent Application No. 2001-176943 discloses a method for detecting stacking faults of epitaxial wafers using an optical scattering method. In this method, using an abnormality detection device employing an optical scattering method (for example a Surfscan 6200 (Trade Mark) manufactured by KLA-Tencor Ltd), the size of laser light scatterers present on the surface of an epitaxial wafer is measured and these laser light scatterers are classified into bodies whose size is no more than 1.6 μm and bodies that exceed this value; laser light scatterers exceeding 1.6 μm are identified as being stacking faults, while laser light scatterers of no more than 1.6 μm are identified as pits other than stacking faults. 
   DISCLOSURE OF THE INVENTION 
   The invention disclosed in Laid-open Japanese Patent Application No. 2001-176943 is subject to the following problems. 
   First of all, defects exist at the wafer surface in a large variety of forms: this makes it difficult to classify such defects in terms of the intensity of the scattered light from a single laser beam with a high degree of certainty. It is even difficult to distinguish between defects and particles. The most that can be achieved with this method is to classify defects into two types, with a threshold value of 1.6 μm. Also, performance of selective etching as pretreatment greatly lowers the throughput of defect inspection, so this method is unsuitable for mass-production and the surface quality of the wafers is impaired by selective etching, to the extent that it may no longer be possible for such wafers to be shipped as products. Further, Laid-open Japanese Patent Application No. 2001-176943 does not discuss classifying laser light scatterers at the wafer surface into killer defects and defects which are not killer defects. 
   An object of the present invention is therefore to improve the accuracy of surface inspection of semiconductor wafers and in particular epitaxial wafers using an optical scattering method. 
   A further object is to improve the accuracy of identification of defects and particles in surface inspection of semiconductor wafers and in particular epitaxial wafers using an optical scattering method. 
   Yet another object is to improve the accuracy of identification of killer defects and defects which are not killer defects in surface inspection of semiconductor wafers and in particular epitaxial, wafers using an optical scattering method. 
   Also, yet another object is to provide an inspection device or method of inspection that is more suited to mass production. 
   A semiconductor wafer inspection device according to one aspect of the present invention comprises: an optical illumination device that directs a light spot onto an inspection point on a surface of the semiconductor wafer; a first optical sensor that, of scattered light from said inspection point, receives narrowly scattered light scattered with a scattering angle that is narrower than a prescribed angle and detects intensity of said narrowly scattered light; a second optical sensor that, of scattered light from said inspection point, receives widely scattered light scattered with a scattering angle that is wider than a prescribed angle and detects intensity of said widely scattered light; and a signal processing circuit that identifies the type of laser light scatterer (LLS) present at said inspection point. Said signal processing circuit comprises: first calculation means that, if the intensity of said narrowly scattered light is within a prescribed sizing range, calculates a first PLS-based size from the intensity of said narrowly scattered light; second calculation means that, if the intensity of said widely scattered light is within said sizing range, calculates a second PLS-based size from the intensity of said widely scattered light; and identification means that, if the intensities of said narrowly scattered, light and said widely scattered light are both within said sizing range, identifies the type of said laser light scatterer in accordance with both the first PLS-based size and said second PLS-based size. 
   In a suitable embodiment, said identification means identifies a laser light scatterer present at said inspection point as being a particle, in a prescribed particle zone in which said first PLS-based size in said sizing range is either substantially equal to said second PLS-based size or is larger than said second PLS-based size, by a degree not more than a prescribed degree. 
   In a suitable embodiment, said identification means identifies a laser light scatterer present at said inspection point as being a defect, in a prescribed defect zone in which said first PLS-based size in said sizing range is larger than said second PLS-based size, by a degree not less than said prescribed degree. In this case, said identification means identifies whether said defect is assumed to be a killer defect or not, in accordance with whether the first PLS-based size is larger or smaller than a prescribed size, in said defect zone. 
   In a suitable embodiment, said identification means identifies a laser light scatterer present at said inspection point as being a defect that is assumed to be a killer defect if the intensity of said, narrowly scattered light or said widely scattered light exceeds said sizing range. 
   A method of inspection of semiconductor wafers according to another aspect of the present invention comprises: a step of directing a light spot onto an inspection point on the surface of the send conductor wafer; a step of detecting the intensity, of the scattered light from said inspection point, of narrowly scattered light scattered with a scattering angle that is narrower than a prescribed angle; a step of detecting the intensity, of the scattered light from said inspection point, of widely scattered light scattered with a scattering angle that is wider than the prescribed angle; a step of, if the intensity of said narrowly scattered light is within a prescribed sizing range, calculating a first PLS-based size from the intensity of said narrowly scattered light; a step of, if the intensity of said widely scattered light is within said sizing range, calculating a second PLS-based size from the intensity of said widely scattered light; and a step of, if the intensities of said narrowly scattered light and said widely scattered light are both within said sizing range, identifying the type of laser light scatterer present at said inspection point in accordance with the magnitude relationship of said, first PLS-based size and said second PLS-based size. 
   According to the present invention, the accuracy of surface inspection of semiconductor wafers using an optical scattering method can be improved. 

   
     BRIEF DESCRIPTION OF THE DRAWINGS 
       FIG. 1A  is a cross-sectional view showing the construction of a semiconductor wafer inspection device according to an embodiment of the present invention;  FIG. 1B  is a plan view showing how scanning of a semiconductor wafer surface is conducted using a light spot; 
       FIG. 2  is a waveform diagram showing a plurality of types of light intensity signal  122 ,  124  output from optical sensors  114 ,  120 ; 
       FIG. 3  is a view showing the most basic principles that are fundamental to the analysis processing for identifying types of surface abnormality, performed by the second signal processing device  126 B; 
       FIG. 4  is a view given in explanation of the logic for identifying types of LLS that is employed in the analysis processing performed by the second signal processing device  126 B; 
       FIG. 5  is a view given in explanation of the theoretical significance of the second EKD zone  420 ; and 
       FIG. 6  is a view showing the flow of analysis processing carried out by the signal processing devices  126 A and  126 B. 
   

   DESCRIPTION OF THE PREFERRED EMBODIMENT 
     FIG. 1A  is a cross-sectional side view showing the construction of a semiconductor wafer inspection device according to an embodiment of the present invention.  FIG. 1B , shown in the dotted line balloon block, is a plan view showing how scanning is performed of the semiconductor wafer surface using a light spot. 
   As shown in  FIG. 1A , this inspection device  100  is capable of selectively directing two laser beams  102 ,  104  onto a point (inspection point) on the surface of a semiconductor wafer  200 . One of the laser beams  102  is directed perpendicularly onto the surface of the semiconductor wafer  200  while the other laser beam  102  is directed onto the surface of the semiconductor wafer  200  at an inclined angle. In this embodiment, only the perpendicularly directed laser beam  102  is employed and the laser beam  104  that is directed in inclined fashion is not employed. The inspection point on the surface of the semiconductor wafer  200  is illuminated by a minute laser-spot  103  that is formed by the perpendicularly directed laser beam  102 . As shown in  FIG. 1B , this laser spot  103  has an elongate elliptical shape; the major diameter and minor diameter thereof face directions that are respectively parallel with the radius and circumferential line of the semiconductor wafer  200 . The size of the laser-spot  103  is for example about 50 to 350 μm in the case of the major diameter dimension L and about 20 μm in the case of the minor diameter dimension W. In the Inspection device  100 , the semiconductor wafer  200  is rotated about the central point as shown by the arrow  200 A of  FIG. 1B  and, simultaneously, the laser spot  103  is moved along the radius of the semiconductor wafer  200  as shown by the arrow  103 A; in this way, the entire region of the surface of the semiconductor wafer  200  is scanned in spiral fashion by the laser spot  103 . The interval between the spiral scanning lines (interval of the Nth scanning line and N+1 th scanning line in the radial direction; is about 20 to 180 μm i.e. about half of the major diameter dimension L of the laser spot  103 . Consequently, the positional resolution of the inspection result obtained by this scanning is about 20 to 180 μm. 
   At the inspection point (location where the light spot  103  is incident) on the semiconductor wafer  200 , the perpendicularly incident laser beam  102  is reflected in a direction depending on the surface condition at this inspection point. For example, if no defect or particle is present at the inspection point, the surface shape at the inspection point is completely flat, so the perpendicularly incident laser beam  102  is reflected, perpendicularly. On the other hand, if a defect or particle is present at the inspection point, since a protuberance or concavity is present in the surface shape, the reflected light from the perpendicularly incident laser beam  102  forms scattered light  108 ,  116  in various directions. The perpendicularly reflected beam from the inspection point is absorbed by the mask  106  and is not employed in inspection. On the other hand, part of the scattered reflected light from the inspection point is detected by the optical sensor  114 , depending on the scattering angle (reflected angle) thereof, while another part thereof is detected by another optical sensor  120 . Specifically, the reflected light  108  that is scattered in a narrow angle range of scattered angle no more than a prescribed value (hereinbelow referred to as “narrowly scattered light”) passes through a convex lens  110  and reflecting mirror  112  and is detected by a first optical sensor  114 . Also, the reflected light  116  that is scattered in a wide-angle range of scattered angle larger than the prescribed angle (hereinbelow referred to as “widely scattered light”) passes through a solid concave reflecting mirror  118  and is detected by a second sensor  120 . The first optical sensor  114  generates an electrical signal  122  (for example, a voltage signal) (hereinbelow referred to as the “narrowly scattered, light intensity signal”) having a level responsive to the intensity of the narrowly scattered light  108  and this is output to the first signal processing device  126 A. The second optical sensor  120  generates an electrical signal (for example, a voltage signal) (hereinbelow referred to as “widely scattered light intensity signal”)  124  having a level responsive to the intensity of the widely scattered light  116  and this is output to the first signal processing device  126 A. For example photomultiplier tubes may be employed for the optical sensors  114 ,  120 . 
   A first and second mutually connected signal processing device  126 A and  126 B are provided. The combination of first and second signal processing devices  126 A and  126 B, by performing analysis by a method described in detail below, of the input narrowly scattered light intensity signal  122  and widely scattered light intensity signal  124 , detects laser light scatterers (hereinbelow referred to as LLS) (these typically correspond to “surface abnormalities” such as for example protuberances or concavities of the wafer surface, in other words, defects or particles) on the surface of the semiconductor wafer  200 , identifies the detected LLS as a particle, a severe defect having a high probability of being a killer defect, or a slight defect having a low probability of being a killer defect, and outputs the results of this identification. The first signal processing device  126 A, using in particular the narrowly scattered light intensity signal  122  and widely scattered light intensity signal  124 , detects laser light scatterers (hereinbelow referred to as LLS) on the surface of the semiconductor wafer  200 , and calculates the size and positional co-ordinates thereof. The second signal processing device  126 B receives data  125  indicating the size and positional co-ordinates of the LLS from in particular the first signal processing device  126 A and identifies whether this LLS is a particle, severe defect or slight defect, and, in accordance with the results of this identification, determines the detection result, i.e. whether the semiconductor wafer  200  is a good product or not, and outputs this determination result and inspection result. Of the output data from the second signal processing device  126 B, data  127  indicating at least the above inspection result is input to the first signal processing device  126 A. The first signal processing device  126 A outputs a sorting instruction signal  128  corresponding to this inspection result to a wafer manipulator  129 . The wafer manipulator  129  sorts the semiconductor wafers  200  whose inspection has been completed into good products and defective products in accordance with the sorting instruction signal  128 . The first and second signal processing devices  126 A and  126 B can respectively be implemented by for example a programmed computer, dedicated hardware circuit or a combination of these. 
   For the portion of this inspection device  100  excluding the second signal processing device  126 B, for example an SP 1  (Trade Mark; manufactured by KLA-Tencor Ltd may be used. This inspection device  100  can therefore be realized by adding the signal analysis function of the second signal processing device  126 B to this SP 1 . 
     FIG. 2  is a waveform diagram showing different types of scattered light intensity signals  122 ,  124  that may be analysed by the signal processing devices  126 A and  126 B. The type shown in  FIG. 2  may be applied to both the widely scattered light intensify signal  122  and narrowly scattered light intensity signal  124 . 
   As shown in  FIG. 2 , the scattered light intensity signals  122 ,  124  that may be analyzed by the signal processing device  126  may be broadly classified into five types, namely,  130 ,  136 ,  138 ,  140  and  142 , depending on the signal level (for example voltage level). The first type  130  is a type in which the peak value of the signal level is within the range of at least a prescribed lower limiting level Min but less than a prescribed maximum level Max. This prescribed lower limiting level Min is the minimum signal level at which it can be recognised that an LLS has been detected (i.e. level at which it cannot be recognized that an LLS exists unless the signal level is at least this value). The maximum level Max is the signal level corresponding to the maximum size in respect of which LLS sizing (calculation of the PLS (polystyrene latex sphere) size based on the signal level) can be performed. The higher the peak values of the respective levels of the scattered light intensity signals  122 ,  124 , the larger is the size that is thus calculated. However, the calculated result is the size of a PLS (hereinbelow referred to as “PLS-based size”) that reflects scattered light of the same intensity as the LLS and is not the size of the LLS itself. Hereinbelow, this first type  130  will foe called “sized LLS type”. 
   The second type  136  is the case where the signal level reaches the saturation level Max. Essentially, the second type  136  is the case in which the intensity of the reflected amounts of light  108 ,  116  exceeds the maximum value in respect of which sizing can be performed. Hereinbelow, the second type  136  will be referred to as the “saturated area type”. Also, one or other of the following third to fifth types  138 ,  140 ,  142  is identified when a condition of a large number of successive signals, or a high density of signals, of the saturated area type  136  or of the sized LLS type  130  described above is detected. 
   The third type  138  represents the case where signals of the sized LLS type  130  or saturated area type  136  described above are successively detected over at least a prescribed number of tracks (for example eight tracks) in the radial direction of the semiconductor wafer  200 . The successively detected signals may be exclusively of the sized LLS type  130  or exclusively of the saturated area type  136 , or may include a mixture of both types  130  and  136 . Successive signals belonging to the third type  138  are referred to hereinbelow as a whole as being of the “track area type”. 
   The fourth type  140  represents the case where signals of the sized LLS type  130  or saturated area type  136  continuing over at least a prescribed distance (for example 180 μm, corresponding to eight successive laser spots  130 ) in the circumferential direction of the semiconductor wafer  200  (i.e. along the line of spiral scanning) are detected. The successively detected signals may foe exclusively of the sized LLS type  130  or exclusively of the saturated area type  136 , or may include a mixture of both types  130  and  136 . Successive signals belonging to the fourth type  140  are referred to hereinbelow as a whole as being of the “angle area type”. 
   The fifth type  142  does not correspond with either the tracking area type  138  or angle area type  140  described above, but represents the case where a plurality of signals of the sized LLS type  130  or saturated area type  136  described above are detected at adjacent positions whose mutual separation is within a prescribed distance. The plurality of signals belonging to the fifth type  142  are referred to hereinbelow as a whole as being of the “cluster area type”. 
   In addition, the tracking area type  138 , angle area type  140  and cluster area type  142  described above are referred to hereinbelow simply by the general term “area type”  144 . 
   Referring once more to  FIG. 1 , whilst scanning of the semiconductor wafer  200  is being performed by the laser spot  103  the first signal processing device  126 A monitors the signal levels of the respective scattered light intensity signals  122 ,  124  and detects the scattered light intensity signals associated with the sized LLS type  130  and saturated area type  136 , and stores the detected signal levels, type and position co-ordinates. In addition, the first signal processing device  126 A, using the positional co-ordinates of the plurality of signals of the detected sized LLS type  130  and saturated area type  136 , detects the scattered light intensity signals belonging to the area type  144  (tracking area type  138 , angle area type  140  and cluster area type  142 ), and calculates the size of the region where such a signal is detected. 
   The second signal processing device  126 B receives from the first signal processing device  126 A data  125  indicating the detection result of the signals of the widely scattered light intensity signal  122  and narrowly scattered light intensity signal  124  of the sized LLS type  130 , the saturated area type  136  and the area type  144  respectively described above and, by analyzing both of these detection results by the method to be described, determines the type of LLS (particle or severe defect or slight defect). 
   A detailed description of the analysis processing for identifying the type of LLS that is performed by the second signal processing device  126 B is given below. 
     FIG. 3  is a view showing the most fundamental principles constituting the basis of this signal processing. 
     FIG. 3A  shows the inferred intensity distribution of the reflected scattered light  108 ,  116  when a PLS  300  is located on the surface of a semiconductor wafer  200 .  FIG. 3B  shows the inferred intensity distribution of the reflected scattered light  103 ,  116  when a particle  302  is located on the surface of a semiconductor wafer  200 .  FIG. 3C  shows the inferred intensity distribution of the reflected scattered light  108 ,  116  when a flat protuberance  304  or shallow concavity  306  (of low height or shallow depth compared with the dimensions of the plane) exists on the surface of the semiconductor wafer  200 .  FIG. 3D  shows the inferred intensity distribution of the reflected scattered light  108 ,  116  when a tower-shaped protuberance  308  (of large height compared with the dimensions of the plane) exists on the surface of the semiconductor wafer  200 . 
   As shown in  FIG. 3A , the PLS  300  is close to a perfectly spherical shape. The inspection device  100  is then calibrated so as to show the precise value of the diameter of an actual PLS  300 , whether the size is calculated from the narrowly scattered light from the PLS  300  or from the widely scattered light from the PLS  300 . As shown in  FIG. 3B , most particles  302  may be considered as having a three-dimensional shape whose planar dimensions and height are roughly balanced, so there is not much difference between the PLS-based size of a particle  302  calculated from the narrowly scattered light  108  and the PLS-based size calculated from the widely scattered light  116 ; or, if the particle  302  is stabilized in a flatfish attitude, the PLS-based size calculated from, the narrowly scattered light  108  may be inferred to be somewhat larger than that calculated from the widely scattered light  116 . Also, as shown in  FIG. 3C , in the case of a flat protuberance  304  or concavity  306 , faces that are close to horizontal will clearly foe wider than faces that are close to vertical, so the PLS-based size calculated from narrowly scattered light  108  will be inferred to be clearly larger than that calculated from widely scattered light  116 . Contrariwise, as shown in  FIG. 3D , in the case of a tower-shaped protuberance  308 , since the faces that are close to vertical will be clearly wider than faces that are close to horizontal, the PLS-based size calculated from the widely scattered light  116  will be inferred to be clearly larger than that calculated from the narrowly scattered light  108 . 
   Taking as an example the case of an epitaxial wafer (semiconductor having a thin epitaxial layer grown on the surface of the semiconductor based substrate), the relationship of defects thereof with the principles of  FIG. 3  will be described with reference in particular to killer defects. 
   Most epitaxial wafer defects are stacking faults (SF) of the epitaxial layer. There are various different types of SF of the epitaxial layer, but, in most types, a flat protuberance  304  or concavity  306  as shown in  FIG. 3C  is formed in the surface of the epitaxial layer. Not all these SF are necessarily killer defects, but, if the size of a protuberance  304  or concavity  306  is more than a certain amount, there is a nigh likelihood that it will constitute a killer defect. For example, if a protuberance  304  or concavity  306  having a pyramidal or mesa-like geometrical three-dimensional shape with a planar dimension of the order of a few μm to a few tens of urn and a height of the order of a few tens of nm to a few hundreds of nm, or a complex three-dimensional shape comprising an irregular mixture of such shapes, is present in the surface of the epitaxial layer, this is deemed, to be a killer defect. Also, if a large number of LLS protuberances or concavities are successively aggregated over a wide region exceeding for example a total length of 100 μm in the surface of the epitaxial layer, this is termed a large area defect (LAD), which is also typically a killer defect. 
   Consequently, if the intensity of the narrowly scattered light  108  is markedly greater than the intensity of the widely scattered light  116 , as shown in  FIG. 3C , at a given detection point on the surface of the epitaxial wafer, a defect is inferred to be present at this detection point. Also, it may be assumed, that the larger the size of such a defect, the greater will be the likelihood of such a defect being a killer defect. Also, if, as shown in  FIG. 3B , the intensity of the widely scattered light  116  and the intensity of the narrowly scattered light  108  at a given detection point are of the same order, or the former is slightly greater than the latter, existence of a particle at the detection point is inferred. Also, when a scattered light intensity signal of an area type  144  as shown in  FIG. 2  is obtained in a given region on the surface of an epitaxial wafer, it is considered as a strong possibility that a defect of correspondingly large size or a LAD is present thereon. 
   In the analysis processing performed by the second signal processing device  126 B, detection/identification logic is employed based on the above principles in order to identify the various types of LLS. 
     FIG. 4  shows an example of this detection/identification logic. 
   The detection/identification logic shown in  FIG. 4  was obtained by the present inventors on the basis of the principles described above with reference to  FIG. 3  and also as a result of repeated studies of inspections of particles or defects of various types on actual epitaxial wafers using an SP1 manufactured by KLA-Tencor Ltd. 
     FIG. 4A  shows the detection/identification logic applied when scattered light intensity signals  122 ,  124  of sized LLS type  130  and saturated, area type  136  as shown in  FIG. 2  were obtained. In  FIG. 4A , the horizontal axis shows the PLS-based size (diameter) DWN calculated using a widely scattered light intensity signal  124  of the sized LLS type  130 ; the right-hand end thereof corresponds to the case where a widely scattered light intensity signal  124  of saturated area type  136  was obtained. In  FIG. 4A , the vertical axis snows the PLS-based size (diameter) DUN calculated using the narrowly scattered light intensity signal  124  of the sized LLS type  130 ; the upper end thereof corresponds to the case where a narrowly scattered light intensity signal  122  of the saturated area type  136  was obtained. Also,  FIG. 4B  shows the detection/identification logic applied in the case where scattered light intensity signals  122 ,  124  of area type  144  shown in  FIG. 2  were obtained. In  FIG. 4B , the horizontal axis shows the size of the region where a widely scattered light intensity signal  124  of the area type  144  was detected and the horizontal axis shows the size of the region where a widely scattered light intensity signal  122  of area type  144  was detected. 
   In a range in which the scattered light intensity signals  124  and  122  shown in  FIG. 4A  are both of the sized LLD type  130  (for example range in which 0.0&lt;DNN&lt; about 0.8 μm, and 0.0&lt;DWN&lt; about 0.6 μm, hereinbelow referred to as the “sizing range”), if a signal analysis result belonging to the zone  410  is obtained from a given detection point, it is also concluded that a particle is present at that detection point. This zone is termed the “particle zone”. 
   The particle zone  410  is a cone sandwiched between a first discrimination line  400  and a second discrimination line  402  in the sizing range and satisfies the conditions that the PLS-based size DIM obtained from widely scattered light  116  is less than about 0.6 μm and that the narrowly scattered light intensity signal  122  has not reached saturation. The first discrimination line  400  corresponds to the case where the PLS-based size OWN obtained from the widely scattered light  116  and the PLS-based size DNN obtained from the narrowly scattered light  108  are substantially of the same order (the PLS-based size DWH obtained from the widely scattered light  116  is slightly smaller than the PLS-based size DNN obtained from the narrowly scattered light  108 ). Hereinbelow, this first discrimination line  400  will be termed the “particle lower limit line”. The particle lower limit line  400  may be expressed by for example a first order function
 
 DNN=K·DWN  
 
   where K is a coefficient between 1 and 0.5, having for example a value of about 0.8 to 0.9. 
   The second discrimination line  402  corresponds to the case where the PLS-based size DNN obtained from the narrowly scattered light  108  is to a certain extent larger than the PLS-based size DWN obtained from the widely scattered light  116 . Hereinbelow, this second discrimination line  402  will be termed the “defect separation line”. The defect separation line  402  may be expressed for example by the function
 
log( DNN )=(1/ S )log( DWN )+ T/S , and DNN≧DWN
 
   Where S and T are positive coefficients of less than 1, having for example values of about 0.4 to 0.6. 
   The particle zone  410  essentially corresponds to the case where the PLS-based size DNN calculated from the narrowly scattered light  108  is of the same order as or is larger than the PLS-based size DWN calculated from the widely scattered light  116 , within a prescribed range, under the condition that both of the narrowly scattered light intensity signal  122  and widely scattered light intensity signal  124  are of the sized LLS type. In this case, the evaluation result is obtained that a particle is present. This evaluation result conforms to the principles described with reference to  FIG. 3B . 
   In the sizing range shown in  FIG. 4A , it is concluded that a slight defect, that is inferred not to be (or unlikely to be) a killer defect, is present at the detection point where an analysis result belonging to the zone  414  was obtained (such a defect is hereinbelow termed a “small defect”). Also, at a detection point where an analysis result belonging to the zone  418  was obtained, it is concluded that a severe structural defect (hereinbelow termed “EKD (estimated killer defect)”) inferred to be (or likely to be) a killer defect is present. The zone  414  is termed the “first small defect zone” and the zone  418  is termed the “first EKD cone”. 
   The first small defect zone  414  and first EKD zone  418  are zones wherein the PLS-based size DWN obtained using the widely scattered light intensity signal  124  is smaller than the defect separation line  402 . Also, the first small defect zone  414  and first EKD zone  418  are distinguished by the third discrimination line  403 . The third discrimination line  403  will hereinbelow be called the “EKD separation line”. The EKD separation line  403  is a line at which for example the PLS-based size DNN obtained using the narrowly scattered light intensity signal  122  corresponds to 0.6 μm. In the first small defect zone  414 , the PLS-based size DNN obtained using the narrowly scattered light intensity signal  122  is less than 0.6 μm and, in the first EKD zone  418 , this signal is more than 0.6 μl. In simple terms, this is a case in which the PLS-based size DNN obtained from the narrowly scattered light  108  is greater by at least a prescribed amount than the PLS-based size DWN obtained using the widely scattered light  116 , in the small defect zone  414  and also the first EKD zone  418 . Also, if the PLS-based size DNN detected using the narrowly scattered light  108  is less than 0.6 μm, it is concluded that a small defect is present; if the PLS-based size DUN is more than 0.6 μm, it is concluded that an EKD is present. This evaluation result is in accordance with the principles described with reference to  FIG. 3C . 
   Also, in the sizing range indicated, in  FIG. 4A , the probability that a zone  430  will actually foe detected is fairly low; it appears that this corresponds to a tower-shaped defect as shown in  FIG. 3D  or to a defect present in the vicinity of an edge. This zone  430  is evaluated as corresponding to a small defect as described above. Such a zone  430  is hereinbelow referred to as a “second small defect zone”. The second small defect zone  430  is a zone in respect of which the PLS-based size DNN obtained using the narrowly scattered light intensity signal  122  is on the small side compared with the particle lower limit line  400 . 
   Furthermore,  FIG. 4A  shows special zones  412 ,  416 ,  417 ,  420 ,  421 ,  423 ,  424 ,  425  and  426  at the outer edge of the first small defect  412 , first EKD zone  413 , particle zone  402  and second small defect zone  430  described above. The significance of these special zones  412 ,  416 ,  417 ,  420 ,  421 ,  423 ,  424 ,  425  and  426  is essentially that these indicate cases where at least one level of the scattered light intensity signals  122 ,  124  is less than the lower limiting level Min shown in  FIG. 2  (i.e. no LLS detected), or that the LLS is of the saturated area type  136 . The special zone  412  adjacent to the first small defect zone is evaluated as corresponding to a small defect. The two special zones  416  and  417  adjacent to the first EKD zone  418  are both evaluated as EKD. The three special zones  420 ,  421  and  423  adjacent to the particle zone  410  are evaluated as EKD. The two special zone levels  424  and  425  corresponding to the saturated area type  136  adjacent to the second small defect zone  430  are also evaluated as EKD. The special zone  426  corresponding to DNN-0.0 μm adjacent to the second defect zone  430  is evaluated as a small defect. 
   However, in the case of the special zone  420  adjacent to the particle zone  410 , the narrowly scattered light intensity signal  122  is of the saturated area type, whereas the widely scattered light intensity signal  124  is of the sized LLS type; this is a case in which the PLS-based size DWN that is thereby obtained is at least 0.3 μm. As shown theoretically in  FIG. 5 , this special zone  420  appears to be a projection region of the particle expansion region  431  on the extension of the particle zone  410  and is also a projection region of the EKD expansion region  432  on the extension of the first EKD zone  418 . Consequently, a particle or EKD may also theoretically foe present in the special zone  420 . However, in practice, this problem can be avoided by choice of a suitable value of the saturation size of the DNN. According to the studies made by the present inventors, by setting the DNN saturation value to about 0.8 μm, it was found that substantially all of the laser light scatterers on the special zone  420  were EKDs. It is therefore concluded that an EKD is present in this special zone  420 . 
   The zone  422  shown in  FIG. 4B  represents the case where both the narrowly scattered optical signal  122  and scattered light intensity signal  124  are of the saturated area type  136  or area type  144  shown in  FIG. 2 . The minimum values of the vertical axis and horizontal axis of this zone  422  are values that are larger than the maximum values of the PLS-based size DNN and DWN that may be calculated using sized LLS type  130  signals, it may be concluded that an EKD as described above is present at the detection point where an analysis result belonging to this zone  422  was obtained. This zone  422  is called the “second EKD zone”. 
     FIG. 6  shows the flow of analysis processing performed using the signal processing devices  126 A and  126 B in surface inspection of a semiconductor wafer. 
   As described with reference to  FIG. 1 , the steps  500 ,  502 ,  504  and  506  shown in  FIG. 6  are continuously executed during scanning of the surface of a semiconductor wafer  200  with a light spot  103 . In the steps  500  and  502 , the narrowly scattered light intensity signal  122  and widely scattered light intensity signal  124  from the current detection point are input simultaneously to the first signal processing device  126 A. In steps  504  and  506 , if the respective signal levels of the narrowly scattered light intensity signal  122  and widely scattered light intensity signal  124  exceed the lower limiting level Min shown in  FIG. 2 , these signal levels and the positional-co-ordinates of the point of detection are stored in a storage device (not shown) within the first signal processing device  126 A. 
   The routine subsequent to steps  508  and  510  may be performed whilst the above scanning is being performed, or may be performed after the above scanning has been terminated. 
   In step  508 , a check is made to ascertain whether the signal, level of the narrowly scattered light intensity signal  122  detected at this position has reached the saturated level Max, or is less than this (i.e. is unsaturated), at each of the positional co-ordinates of the detection points stored in the storage device in the first signal processing device  126 A. In step  510 , a check is made to ascertain whether the signal level of the widely scattered light intensity signal  124  detected at this position has reached the saturation level Max, or is less than this (i.e. is unsaturated), at each of the positional co-ordinates of the detection points stored in the storage device in the signal processing device  126 . 
   In step  512 , if the result of the check of step  508  is “unsaturated” (i.e. that the narrowly scattered light intensity signal  122  is of the sized LLS type  130 ), the PLS-based size DNN is calculated based on the signal level of this narrowly scattered light intensity signal  122 , and the PLS-based size DNN is stored in the storage device in association with the positional co-ordinates of the corresponding detection point. In step  514 , if the result of the check of step  510  is “unsaturated” (i.e. that the widely scattered light intensity signal  124  is of the sized LLS type  130 ), the PLS-based size DWN is calculated based on the signal level of this widely scattered light intensity signal  124 , and the PLS-based size DWN is stored in the storage device in association with the positional co-ordinates of the corresponding detection point. 
   In step  516 , a check is made to ascertain whether a narrowly scattered light intensity signal  122  is present corresponding to the saturated area type  136  and area type  144  and the result of this check is stored in the storage device in association with the positional co-ordinates of the corresponding point of detection. In step  518 , a check is made to ascertain whether a widely scattered light intensity signal  124  is present corresponding to the saturated area type  136  and area type  144  and the result of this check is stored in the storage device in association with the positional co-ordinates of the corresponding point of detection. 
   In step  520 , if the result of the check performed in step  516  indicates area type  144 , the size of the region where a narrowly scattered light intensity signal  122  of this area type  144  was detected is calculated using the positional co-ordinates of the plurality of corresponding detection points and the size of this region is stored in the storage device in association with the positional co-ordinates of the corresponding detection points. In step  522 , if the check result of step  518  indicates area type  144 , the size of the region where the widely scattered light intensity signal  124  of this area type  144  was detected is calculated, using the positional co-ordinates of the plurality of corresponding detection points, and the size of this region is then stored in the storage device in association with the positional co-ordinates of the corresponding detection points. 
   In step  524 , data indicating the positional co-ordinates of the detection points stored in the storage device, the PLS-based size DNN or region size obtained using the narrowly scattered light intensity signal  122 , and the PLS-based size DWN or region size obtained using the widely scattered light intensity signal  124  are transferred to the second signal processing device  126 B. The second signal processing device  126 B uses this data to evaluate, in accordance with the detection/evaluation logic already described and shown in  FIG. 4 , at which positions on the semiconductor wafer  200  an LLS is present or not, and, if an LLS is present, whether this LLS is a particle, small defect or EKD. This evaluation result is stored in the storage device in association with the positional co-ordinates of the corresponding detection point and whether or not the semiconductor wafer  200  is satisfactory is decided in accordance therewith. The results of these evaluations or decisions are output to the outside for display of the detection results or in order for further analysis to be performed, and the wafer manipulator  129  separates the semiconductor wafers  200  in accordance with the results of this decision regarding suitability. 
   With the inspection device  100  and inspection method described above with reference to the drawings, inspection can be performed even though no selective etching of the surface of the semiconductor wafer  200 , such as was performed prior to inspection in the conventional inspection method, has been carried out. This inspection device  100  and inspection method are therefore suitable for application to mass-production. 
   While embodiments of the present invention have been described above, these embodiments are merely given by way of example for explanation of the present invention and the scope of the present invention is not intended to be restricted solely to these embodiments. The present invention can be put into practice in various other modes, without departing from its essence.