Abstract:
As circuit patterns become finer in recent years, improvement in detection sensitivity of defects is required. To answer this, sensitivity is being enhanced using a laser with a wavelength of the UV band as the laser for irradiation. A pulse oscillation laser is often used as the UV laser. However, a peak (maximum output) of the pulse oscillation laser becomes very large to an average output power required. For example, in the case of a laser of average output power 2 W, pulse interval 10 ns, and pulse width 10 ps, the peak (maximum output) becomes as high as 2 kW, and there is the possibility of causing a damage to a sample. Therefore, it is necessary to reduce the peak (maximum output) with the average output power being maintained, so that it may not cause a damage to the sample. In this invention, the device is configured in such a way that pulsed light is optically divided into several pulses and these pulses are given respective paths whose lengths are set different from one another, whereby the peak (maximum output) is reduced while the average output value are maintained.

Description:
BACKGROUND OF THE INVENTION  
       [0001]     1. Field of the Invention  
         [0002]     This invention relates to a foreign matter and defect detecting apparatus for detecting minute foreign matters and/or defects existing on a semiconductor substrate etc. with high sensitivity and high speed.  
         [0003]     2. Description of the Related Art  
         [0004]     In production lines of semiconductor substrates, thin film substrates, etc., in order to maintain and improve product yield, there is widely carried out inspection of defects and foreign matters existing on surfaces of semiconductor substrates, thin film substrates, etc. For example, with a sample of a semiconductor substrate etc. before formation of a circuit pattern, it is necessary to detect minute defects and foreign matters (hereinafter referred to as defects) of a size of 0.05 μm or less on the surface. In the conventional inspecting apparatus, in order to detect such defects, a laser beam of visible light converged to a diameter of a few tens of μm is applied onto the sample surface, and scattered light from the defects are collected and detected. Moreover, with a sample of a semiconductor substrate etc. after circuit pattern formation, the defects are recognized by irradiating a collimated laser beam on the sample surface, collecting the scattered light generated on the sample surface, while diffracted light from a periodical pattern is shaded with a spatial filter, scattered light from the non-periodical pattern and defects is detected, and signals resulting from the non-periodical pattern is eliminated by die comparison.  
         [0005]     As an inspecting apparatus that uses UV light having a shorter wavelength than the visible light as a light source, JP 2003-130808 A discloses a method for irradiating a sample using a UV pulsed laser as a light source with a reduced peak of the pulse and an apparatus therefor.  
       SUMMARY OF THE INVENTION  
       [0006]     In recent years, as circuit patterns become finer, improvement of detection sensitivity of defects is demanded. For this purpose, enhancing sensitivity is tried to be attained using a laser having a wavelength in the UV band as a laser for irradiation. Because the quantity of scattered light generated by minute particles of 0.1 μm or less is in inverse proportion to the fourth power of the irradiation wavelength, enhancing sensitivity becomes possible by shortening the wavelength.  
         [0007]     As a UV laser, a pulse oscillation laser is often used. However, a peak of the pulse oscillation laser (maximum output) becomes highly large to an average output power that is needed. For example, in the case of a laser of average output power 2 W, light emission frequency 100 MHz, pulse interval 10 ns, and pulse width 10 ps, the peak (maximum output) becomes as high as 2 kW and there is the possibility of causing a damage to a sample. For this reason, it is desirable to reduce the peak (maximum output) while maintaining the average output power.  
         [0008]     JP 2003-130808 A discloses a technique of dividing a laser beam emitted from a UV pulsed-laser light source into a plurality of pulses and irradiating them on a sample. However, in JP 2003-130808 A, peaks of the respective divided pulses are set to be reduced gradually, and it was not considered that the maximum of the peak of each pulse after the division was reduced to be as low as possible.  
         [0009]     In this invention, the apparatus for detecting defects is configured to be able to divide a laser beam emitted from the UV pulsed-laser light source into a plurality of pulses and apply each pulse on the sample after the division with a maximum of the peak being reduced to be as less as possible.  
         [0010]     That is, in this invention, in order to be able to inspect defects of a sample without damaging the sample even when using a pulse oscillation UV laser, the apparatus for detecting defects is configured to comprise: laser-beam light source means; irradiation optical system means for irradiating a laser beam emitted from the laser-beam light source means on the sample obliquely; detection optical system means for collecting and detecting scattered light from the sample irradiated by the irradiation optical system means; and signal processing means for processing a signal obtained by detecting the scattered light from the sample by the detection optical system means to detect defects of the sample; wherein the laser-beam light source means emits a ultraviolet pulsed laser beam, and the irradiation optical system means divides each pulse of the pulsed laser beam emitted from the laser beam light source into a plurality of pulses, and this plurality of pulses divided from the pulsed laser beam are transformed into linearly polarized light and applied onto the sample.  
         [0011]     Moreover, an apparatus for detecting defects, comprises: laser-beam light source means; irradiation optical system means for shaping a laser beam emitted from the laser-beam light source means and irradiating it onto a linear area on the sample; detection optical system means for forming an optical image with reflected light from the linear area of the sample irradiated by the irradiation optical system means and taking an optical image thus formed; and signal processing means for processing the image obtained by taking the optical image by the reflected light from the sample by the detection optical system to detect defects of the sample, and the apparatus for detecting detects is configured in such a way that the laser-beam light source means emits an ultraviolet pulsed laser beam, and the irradiation optical system means divides each pulse of the pulsed laser beam emitted from the laser beam light source into a plurality of pulses and shapes this plurality of pulses divided from the pulsed laser beam and apply them onto the linear area on the sample.  
         [0012]     Furthermore, the apparatus that detects defects by irradiating a pulsed laser beam emitted from the pulsed laser beam light source on a sample from an oblique direction, detecting the reflected light from the sample irradiated with the pulsed laser beam from the oblique direction, and processing the signal obtained by detecting the reflected light from the sample is configured in such a way that each pulse of the pulsed laser beam emitted from the laser beam light source is divided into a plurality of pulses and this plurality of pulses of the pulsed laser beam are transformed into linearly polarized light and applied on the sample.  
         [0013]     According to this invention, when using a UV laser of pulse oscillation as an irradiation light source, it is possible to reduce a maximum of the peak of the pulse to be applied on a sample by dividing a pulsed beam emitted from the pulsed laser beam light source into a plurality of pulses and making the peaks of this plurality of pulses divided therefrom to be almost the same value, and therefore, it becomes possible to inspect minute foreign matters and defects with stable sensitivity while reducing damages to the sample.  
         [0014]     These and other objects, features and advantages of the invention will be apparent from the following more particular description of preferred embodiments of the invention, as illustrated in the accompanying drawings. 
     
    
     BRIEF DESCRIPTION OF THE DRAWINGS  
       [0015]      FIG. 1  is a block diagram showing an outline configuration of a first embodiment of an apparatus for detecting defects according to this invention.  
         [0016]      FIG. 2  is a front view showing an outline configuration of a pulsed-light division optical system.  
         [0017]     An upper part of  FIG. 3  shows a time waveform of pulsed light emitted from the laser light source, and a lower part thereof shows a time waveform of pulsed light after the pulsed light is divided by the pulsed-light division optical system.  
         [0018]      FIG. 4  is a front view showing an outline configuration of the pulsed-light division optical system and explaining ellipticity of the pulsed light having passed through the pulsed-light division optical system.  
         [0019]      FIG. 5  is a front view showing an outline configuration of the pulsed-light division optical system that is configured to control a polarization state of a pulsed light having passed through the pulsed-light division optical system.  
         [0020]      FIG. 6  is a front view showing an outline configuration of the pulsed-light division optical system for dividing one pulse into four pulses.  
         [0021]     In  FIG. 7 , the upper part shows a state of pulsed light emitted from the laser light source, and the lower part shows pulsed light after being divided by the pulsed-light division optical system of  FIG. 6 .  
         [0022]      FIG. 8  is a front view showing an outline configuration of a pulsed-light division optical system for dividing one pulse into eight pulses.  
         [0023]      FIG. 9  shows an example of multidirectional irradiation.  
         [0024]      FIG. 10  is a block diagram showing an outline configuration of an irradiation system and a detection system of another example of the multidirectional irradiation.  
         [0025]      FIG. 11  is a block diagram showing an outline configuration of an irradiation system and a detection system of further another example of the multidirectional irradiation.  
         [0026]      FIG. 12  is a front view showing an outline configuration of a modification example of the pulsed-light division optical system.  
         [0027]      FIG. 13  is a front view showing an outline configuration of the pulsed-light division optical system equipped with a function of selecting the number of division of pulse.  
         [0028]      FIG. 14  is an explanatory figure of a GUI screen on which peak reduction is selected.  
         [0029]      FIG. 15  is a perspective view showing an outline configuration of a second embodiment of the apparatus for detecting defects according to this invention.  
         [0030]      FIG. 16  is a perspective view of a linear oblique irradiation unit of the irradiation optical system and a wafer in the second embodiment of the apparatus for detecting defects according to this invention. 
     
    
     DESCRIPTION OF THE PREFERRED EMBODIMENTS  
       [0031]     Hereafter, embodiments of this invention will be described.  
         [0000]     First Embodiment  
         [0032]     An example in which this invention is applied to an apparatus for detecting defects on the surface of a wafer that did not undergo pattern formation.  
         [0033]      FIG. 1  shows one example of an apparatus for detecting defects on a semiconductor wafer before formation of a circuit pattern.  FIG. 1  illustrates an outline configuration of the apparatus, which is constructed to comprise an irradiation optical system  102 , a detection optical system  103 , a wafer stage  101 , a signal processing unit  104 , and a control unit  105 . The irradiation optical system  102  is composed of a laser light source  2 , an attenuator  3 , a beam expander  4 , a pulsed-light division optical system  5 , and a converging lens  7 . The laser light source  2  is a pulse oscillation laser of a wavelength in the UV (Ultra Violet) region (wavelength region of 400 nm or less). A laser beam  201  emitted from the laser light source  2  is controlled so as to have necessary quantity of light by the attenuator  3 , enlarged in beam diameter by the beam expander  4 , reduced in peak by the pulsed-light division optical system  5 , and subsequently converged and applied onto a detection area on the wafer  1  by the converging lens  7 . Mirrors  6   a ,  6   b  change an irradiation light path and are used as required.  
         [0034]     The detection optical system  103  is composed of a scattered-light detection lens  8  and a photoelectric transducer  10 , and uses the scattered-light detection lens  8  to collect almost the whole portion of scattered light  9  from foreign matters on a light receiving surface of the photoelectric transducer  10 . Regarding optical processing of the scattered light, for example, by disposing a polarizing plate and a spatial filter between a wafer  1  and the scattered-light detection lens or between the scattered-light detection lens  8  and the photoelectric transducer  10 , the optical characteristic can be altered/adjusted, or modified otherwise. The photoelectric transducer  10  generates an electric signal whose magnitude is proportional to the quantity of scattered light. By processing this signal in the signal processing circuit  104 , foreign matters and defects are detected and their sizes and locations are found. The photoelectric transducer  10  is used in order to receive and photoelectric-convert the scattered light converged by the detection optical system  103 . In the case where the detection optical system  103  is constructed with an imaging optical system, a TV camera, a CCD linear sensor, or a TDI sensor is used; in the case where it is constructed with a converging optical system, a photomultiplier is used.  
         [0035]     The wafer stage  101  is composed of a chuck (not shown) for holding the wafer  1 , a rotating mechanism (not shown) for rotating the wafer  1 , and a translating mechanism (not shown) for translating the wafer  1  in a radial direction. By the wafer stage  101  rotating the wafer  1  in the horizontal plane and translating it in a horizontal direction, it becomes possible to detect foreign matters and defects and their sizes on the whole area of the wafer  1 .  
         [0036]     The attenuator  3  of this irradiation optical system  102  is constructed with the quarter-wave plate and the polarizing beam splitter (not shown). The emitted beam (linearly polarized light) from the laser light source  2  is transformed into elliptically polarized light by the quarter-wave plate, altering the quantity of light passing through the PBS. By rotating the quarter-wave plate, ellipticity of the polarized light is changed, and accordingly the quantity of light can be adjusted. The beam expander  4  is for enlarging the laser beam  201  emitted from the laser light source  2  in diameter of a cross section perpendicular to an optical axis of the laser beam  201  using a lens system.  
         [0037]     The pulsed-light division optical system  5  is constructed with quarter-wave plates  21   a ,  21   b , PBS&#39;s  22   a ,  22   b , and mirrors  23   a ,  23   b , as shown in  FIG. 2 . The laser beam  201  that is enlarged by the beam expander  4  and enters as linearly polarized light (in this example, P polarized light) is transformed into elliptically polarized light by the quarter-wave plate  21   a , and divided into P polarized light and S polarized light by the polarizing beam splitter  22   a . Ppolarized light, one of the divided polarized lights passes through the polarizing beam splitter  22   a  and the polarizing beam splitter  22   b . An S polarized component, the other of the divided polarized lights is reflected by the polarizing beam splitter  22   a , the mirror  23   a , the mirror  23   b , and the polarizing beam splitter  22   b , respectively, and returns to the same optical axis as that of a P polarized component having passed through the polarizing beam splitters  22   a  and  22   b . At this time, there occurs an optical path difference of Lm between the S polarized component and the P polarized component, where L/2 m is a spacing between the polarizing beam splitter  22   a  and the mirror  23   a  and between the polarizing beam splitter  22   b  and the mirror  23   b . Designating the velocity of light by c(m/s), there occurs a time difference between the S polarized component and the P polarized component as written by an expression below.
 
 t ( s )= L ( m )/ c ( m/s )  (Expression 1)
 
 That is, the pulsed light can be time-divided as shown in  FIG. 3 , and the peak can be reduced to one half. 
 
         [0038]     For example, in the case where a laser of pulse interval 10 ns (10-8 seconds) and pulse width 10 ps (10-11 seconds) and the spacings between the polarizing beam splitter  22   a  and the mirror  23   a  and between the polarizing beam splitter  22   b  and the mirror  23   b  are set to 15 cm (0.15 m), respectively, the time difference between the S polarized component and the P polarized component becomes 1 ns (10-9 seconds). That is, the laser beam with a half peak will be applied on the wafer surface two times at an interval of 1 ns during 10 ns.  
         [0039]     By adjusting the angle of rotation of the quarter-wave plate  21   a , the ratio of the S polarized component and the P polarized component of the incident beam on the polarizing beam splitter  22   a  is set to 1:1. Because of losses (reflectance, transmittance) of optical components used (the polarizing beam splitters  22   a ,  22   b  and the mirrors  23   a ,  23   b ), a peak of the pulsed light may differ between the S polarized component and the P polarized component in the outgoing beam of the polarizing beam splitter  22   b . In order to lower a maximum of the peak of each pulsed light, it is necessary to adjust the peak of each pulsed light to the almost same magnitude. As shown in  FIG. 4 , the P polarized component is only affected by P polarization transmittances (Tp) of the polarizing beam splitters  22   a ,  22   b , whereas the S polarized component is affected by both the S polarization reflectances (Rs&#39;s) of the polarizing beam splitters  22   a ,  22   b  and the S polarization reflectances (Rm) of the mirrors  23   a ,  23   b . Designating S polarized component loss by Ls and designating P polarized component loss by Lp, the loss ratio (Pl) is written by
 
 Pl=Ls/Lp=Rm   2   ×RS   2   /Tp   2 .  (Expression 2)
 
         [0040]     Therefore, by adjusting the angle of rotation of the quarter-wave plate  21   a  so that the ellipticity of the polarization of the incident beam on the polarizing beam splitter  22   a  may become equal to the above-mentioned loss ratio, the peak value can be made almost equal between pulsed light of the S polarized component and the P polarized component of the outgoing beam of the polarizing beam splitter  22   b . The pulsed lights of the P polarized component and the S polarized component so divided that this peak may become almost equal pass through the quarter-wave plate  21   b  and are transformed into circularly polarized light.  
         [0041]     On the other hand, in the inspecting apparatus shown in  FIG. 1 , normally linearly polarized light is used as the laser beam for irradiating the wafer  1 . The laser beam  201  that is transformed into circularly polarized light by the quarter-wave plate  21   b  can be made to be composed of only the P polarized component by making it pass through a polarizing beam splitter  24 , as shown in  FIG. 5 . Since a reflected S polarized component may act as stray light, it is shaded by a beam trap  25 . The peak of the P polarized component that is divided by the polarizing beam splitter  24  and passes through the polarizing beam splitter  24  becomes one half of the peak of the circularly polarized light being incident on the polarizing beam splitter  24 . Therefore, the peak of the P polarized component having passed through the polarizing beam splitter  24  is reduced to one fourth compared with the peak of the pulsed laser beam emitted from the laser light source  2 .  
         [0042]     When using only an S polarized light, what is necessary is to insert a half-wave plate (not shown) after the polarizing beam splitter  24  to effect rotation of polarization direction by 90°. Alternatively, what is necessary is just to rotate the polarizing beam splitters  24  about the optical axis by 90° (in this case, the insertion position of the beam trap  25  is also changed). If the polarization direction is arbitrary, what is necessary is just to use the outgoing beam of the polarizing beam splitter  22   b  as it is.  
         [0043]     In the above description, a method for dividing a pulsed light into two was explained. A method for dividing into four and a method for dividing into eight will be explained with reference to  FIG. 6  and  FIG. 8 , respectively. The configuration shown in  FIG. 6  is a two-stage configuration in which the configuration shown in  FIG. 2  is doubly layered. A spacing between a second-stage polarizing beam splitter  22   c  and a mirror  23   c  and a spacing between a polarizing beam splitter  22   d  and a mirror  23   d  are set to two times the spacing between the first-stage polarizing beam splitter  22   c  and the mirror  23   c  and the spacing between the beam splitter  22   d  and the mirror  23   d , respectively. Emitted beams from the first-stage polarizing beam splitter  22   b  is P polarized pulsed light and S polarized light with a time delay to the P polarized light. By transforming this pulsed light train to circularly polarized light with the quarter-wave plate  21   b , the pulsed light train having passed through the quarter-wave plate  21   b  of an intensity of one half is transformed into P polarized light and passes through the polarizing beam splitters  22   c ,  22   d ; whereas the pulsed light train having passed through the quarter-wave plate of an intensity of one half is transformed into S polarized light, reflected by the polarizing beam splitters  22   c ,  22   d  and by the mirrors  23   c ,  23   d , and returned to the same optical axis. By this optical circuit, the pulsed light is divided into four and each peak is reduced to one fourth, as shown in  FIG. 7 . Strictly, since the optical parts have losses as described above, each peak decreases to be lower than one fourth.  
         [0044]     The P polarized pulsed laser light having passed through the polarizing beam splitter  22   d  and the S polarized pulsed laser light being reflected thereby proceed on the same optical axis to enter a quarter-wave plate  21   c , and are emitted from the quarter-wave plate  21   c , being transformed into circularly polarized light, respectively. This circularly polarized light enters the polarizing beam splitter  24  shown in  FIG. 5  and is divided into the P polarized component and the S polarized component. The P polarized component is applied on the wafer  1  (the peak of the pulsed beam of the P polarized component divided by the polarizing beam splitter  24  becomes one eighth).  
         [0045]      FIG. 8  shows a configuration in which the number of division is further increased. That is, the configuration is changed to be of a three-stage type by further adding a configuration of  FIG. 2  to the configuration of  FIG. 6 . A spacing between a polarizing beam splitter  22   e  ( 22   f ) and a mirror  23   e  ( 23   f ) is set to four times the spacing of the first stage. By this setting, by the same operation as the operation explained in the two-stage configuration, the pulsed light is further divided and the peak is reduced to one-eighth. By further increasing the number of stages, the peak can be reduced to 1/16, 1/32, 1/64, . . . . Restraints in the above-mentioned embodiment are the following two points. The first point is that an optical path difference (L) of the first stage shall be longer than the coherence length (Λ) of the laser beam used, as written by Expression 3,
   L&gt;λ=λ 2/Δλ  (Expression 3) 
 where λ is a wavelength and Δλ is a wavelength bandwidth. The second point is that the divided pulsed light train shall fall within an oscillation interval of the laser, as written by Expression 4,
   L ( n +1)&lt; c ·(1/ f )  (Expression 4) 
 where L is an optical path difference of the first stage, n is the number of stages, c is the velocity of light, and f is an oscillation frequency of the laser. 
 
         [0046]     Although, in the above-mentioned explanation, a polarization component that is not necessary to obtain linearly polarized light finally is shaded with the beam trap  25 , that polarization component can be used for irradiation from two directions, as shown in  FIG. 9 . For example, in the configuration shown in  FIG. 9 , a polarizing beam splitter  30  is inserted instead of the polarizing beam splitter  24  in  FIG. 5 , the P polarized component from the beam in the form of circularly polarized light is made to pass through it and reflected by mirrors  5   c ,  5   d  so as to be applied on the wafer  1  obliquely. On the other hand, the S polarized component is configured to be reflected by the polarizing beam splitter  30 , transformed into P polarized light by a half-wave plate  31 , reflected by a mirror  5   b , and applied on the wafer  1  obliquely from anther direction.  
         [0047]     Regarding an irradiation direction, both of the two beams are made to be incident on the wafer obliquely at almost the same incidence angle, as shown in  FIG. 9 . Moreover, depending on an application, the two beams may be set to be incident at different incidence angles. At this time, one of the beams may be incident from a direction almost perpendicular to the wafer  1 . Moreover, although the laser beam  201  emitted from the laser light source  2  is finally divided into the two beams and applied on the wafer, the two beams may be divided into three or four and used for irradiation. Moreover, a combination of polarized lights can be freely set by a location of the half wave plate  31  (including selection of use or nonuse).  
         [0048]     Since, according to this embodiment, a UV pulsed laser beam can be applied on a wafer with its peak being reduced, it becomes possible to detect extremely minute defects smaller than 0.1 μm without damaging the wafer.  
         [0049]     Next, a method for discriminating irregularities of a defect by applying pulsed laser beams divided by a pulsed-light division optical system on the wafer  1  from multi directions will be explained. As shown in  FIG. 10 , the polarizing beam splitter  30  divides the beam into P polarized light and S polarized light. The S polarized light, one of the divided polarized lights is transformed into P polarized light by the half-wave plate  31 , and irradiation of each pulse beam on the wafer  1  is changed over by opening and shutting of the shutters  32 ,  33 , whereby the wafer  1  is irradiated from two directions having different incidence angles. That is, first, with the shutter  33  being shut, the shutter  32  is opened and the rotating wafer  1  is irradiated with light through the shutter  32 . The whole surface of the sample is inspected by moving an irradiation location of the laser beam relatively in a radial direction of the wafer  1  in conformity with rotation of the wafer  1 .  
         [0050]     Scattered light generated during the inspection is converged by a converging lens  7   a , and the scattered light  8   a  thus converged is detected by a photoelectric transducer  9   a  in synchronization with rotation of the wafer  1 . The detected signal undergoes necessary amplification, noise processing, analog-digital conversion in the analog processing circuit  35   a . When a defect exists, its detection voltage and existence location (location in an R-Θ coordinate system) are stored in the memory  36   a . Subsequently, with the shutter  32  being closed, only the shutter  33  is opened, and the detection is performed. When a defect exists similarly, its detection voltage and existence location are stored in the memory  36   b . When two inspections are ended, contents of the memory  36   a  and contents of the memory  36   b  are compared: that is, detected voltages of a defect in the same coordinates (tolerance included) are compared to discriminate irregularities. Although in  FIG. 10 , the detection system is explained as with two systems, if the apparatus has two pieces of memory  36  separately, the detection system may be with one system.  
         [0051]      FIG. 11  shows another embodiment of a method for discriminating irregularities. The configuration shown in  FIG. 11  is the configuration as shown in  FIG. 10  from which the half-wave plate  31  is removed. With such a configuration, the S polarization irradiation and the P polarization irradiation are simultaneously performed, and it becomes possible to determine irregularities by detecting the scattered light generated from the surface of the wafer  1  with a polarizing plate  38   a  and with a polarizing plate  38   b  independently and comparing these outputs.  
         [0052]      FIG. 12  shows another embodiment of the pulsed-light division optical system  5 . In this embodiment, in the configuration of the apparatus shown in  FIG. 1 , the pulsed-light division optical system  5  is substituted with a quartz block  39  (in the case of visible light, optical glass is also usable), and the pulsed beam that was enlarged in cross section by the beam expander  4  is made to enter this quartz block  39  and to divide a single pulse of a laser beam emitted from the laser light source  2  into a plurality of pulses. The number of block stages composed of this quartz block  39  is made equal to the number of division by which a signal pulse of the laser beam  201  emitted from the laser light source  2  is divided, and the lengths of the blocks is set to have a difference of L′. Designating refractive index of quartz by n, the optical path difference between the blocks becomes L′·(n−1), which will come under restrictions of Expressions (3) and (4). Since the laser beam for irradiation is of a Gaussian distribution  38  and normally the center has higher intensity, the thickness of the block is so changed that the quantity of light passing through each block is made equal.  
         [0053]     In the pulsed-light division optical system  5 ″ of the inspecting apparatus shown in  FIG. 8 ,  FIG. 13  shows an embodiment in which the number of division of the pulsed light is changed in conformity with an inspection target. In  FIG. 13 , the case where a pulsed-light division optical system  5 ′″ is constructed with three stages will be explained. This embodiment is configured to be able to select the number of division of pulsed light by placing or removing mirrors at an input or output position of each stage. For example, if a pair of mirrors  39   a ,  39   b  is inserted before the polarizing beam splitter  22   a , a single pulse of the laser beam  201  emitted from the laser light source  2  is applied on the wafer  1  without being divided. Moreover, if a pair of mirrors  40   a ,  40   b  is inserted before the polarizing beam splitter  22   c , a single pulse of the laser beam  201  emitted from the laser light source  2  is divided and a two-divided pulse train is obtained. Furthermore, if an insertion position of a pair of mirrors is changed to be before the polarizing beam splitter  22   e  or after the polarizing beam splitter  22   f , similarly, a four-divided pulse train or eight-divided pulse train is obtained, respectively.  
         [0054]     Moreover, by enabling the number of division to be selected on a GUI screen  43  as shown in  FIG. 14 , the number of division that matches a sample to be inspected can be set up.  
         [0000]     Second Embodiment  
         [0055]      FIG. 15  shows an example in which this invention is applied to an apparatus for inspecting a wafer on which a pattern has been formed. An irradiation optical system  152  is almost of the same configuration as that shown in  FIG. 1 . That is, the irradiation optical system  152  has the laser light source  2 , the attenuator  3 , the beam expander  4 , the pulsed-light division optical system  5 , the mirrors  6   a ,  6   b  for selecting an irradiation light path, and a converging lens  1501 . The pulsed-light division optical system  5  can also take such a configuration as is explained in  FIGS. 6, 8 , or  13 .  
         [0056]     A detection optical system  153  has a Fourier transform lens  1502 , a spatial filter  1503 , an inverse Fourier transform lens  1504 , and a photoelectric transducer  1505 . For the photoelectric transducer  1505 , a CCD sensor or TDI sensor is used. A signal processing unit  1506  processes a signal detected by the photoelectric transducer  1505  and thereby defects are detected.  
         [0057]     An irradiation area  200  on the wafer  1  irradiated by the irradiation optical system  152  takes the shape that is longer in one direction than in other direction (hereinafter referred to as linear) in conformity with a detection field of view of the detection optical system  153 . Specifically, this linear irradiation area  200  takes the shape of an area elongated in the Y direction perpendicular to the X direction along which a table  151  moves continuously.  
         [0058]      FIG. 16  shows one embodiment of an optical system that realizes liner irradiation. The cylindrical lens  1501  shown in  FIG. 16  allows the laser beam  201  that is enlarged in a diameter of a section perpendicular to the optical axis by the beam expander  4  of the irradiation optical system  152  shown in  FIG. 15  and is divided into a plurality of pulses (for each input pulse) by the pulsed-light division optical system to enter itself, collects them in one direction, converts to a collimated beam in a direction perpendicular thereto, and applies the collimated beam on the wafer  1 . At this time, by setting the laser beam emitted from the cylindrical lens  1501  to be applied on the wafer  1  with an angle φ to the X axis direction of the wafer  1 , a portion of diffracted light from a pattern of linear lines along the X direction or the Y direction on the wafer  1  in  FIG. 16  entering the Fourier transform lens  1502  can be reduced in quantity (because the majority of patterns on the wafer  1  run in directions making 0° or 90° to the X axis direction of the wafer  1 ). In order to perform irradiation along the centerline of the sample, the cylindrical lens  1501  whose focal length varies continuously that has an angle φ and an elevation angle α to a sample centerline is used. The sample  1  undergoes whole surface inspection being scanned with a XYZΘ stage.  
         [0059]     A method for detecting defects on the wafer  1  on which a pattern has been formed using the optical system explained with reference to  FIG. 15  will be explained.  
         [0060]     First, the pulsed laser beam  201  emitted from the laser light source  2  is enlarged by the beam expander  4  in diameter of a cross section perpendicular to the optical axis. One pulse of the beam  201  is divided into a plurality of pulses by any one of the pulsed-light division optical system  5  shown in  FIG. 2 , the pulsed-light division optical system  5 ′ shown in  FIG. 8 , and the pulse-light division optical system  5 ″ shown in  FIG. 13  and incident on the cylindrical lens  1501  after the division. Then the pulses are applied onto a linear area with a longitudinal axis lying in the Y direction on the wafer  1  placed on the table  151  that is controlled by a control unit  1507  and continuously moved in the X direction.  
         [0061]     This irradiation generates scattered light from the wafer  1  on which the pattern has been formed. Diffracted light from a pattern having a comparatively short period pitch, for example, a pattern in a memory part, among patterns formed on the wafer  1  forms a diffracted light pattern on a Fourier transform plane of the Fourier transform lens  1502 . This diffracted light pattern is shaded with a spatial filter  1503  disposed at the Fourier transform plane of the Fourier transform lens  1502 . On the other hand, scattered light from a long period pattern of the order of a die pitch of a large number of dies that are formed on the wafer  1  as well as random scattered light from defects etc. are formed into an image by the inverse Fourier transform lens  1504  without being shaded by the spatial filter  1503 . This optical image thus formed is detected by the photoelectric transducer  1505  in synchronization with movement of the table  151  in the X direction. That is, each time the formed optical image moves by 1 pixel pitch on the photoelectric transducer  1505 , the photoelectric transducer  1505  picks up an optical image.  
         [0062]     In the signal processing unit  1506  connected to the photoelectric transducer  1505 , defects are detected by eliminating information of a long period pattern that has not been erased by the spatial filter  1503  by die comparison, namely, by comparing an image that the photoelectric transducer  1505  has obtained by detection in synchronization with movement of the table  151  in the X direction and image picked up in a location where the same pattern is formed in an adjacent die or neighboring die and stored.  
         [0063]     Note here that since the pulsed laser beam  201  applied on the wafer  1  is a UV laser whose wavelength is shorter than 400 nm, resolution of foreign matter detection improves compared with the case where visible light is used, which enables foreign matter defects whose sizes are less than 0.1 μm to be detected by differentiating them from a pattern formed on the wafer  1 . Further, in this case, since each pulse of the pulsed laser beam  201  emitted from the laser light source  2  is divided into a plurality of pulses by the pulsed-light division optical system  5 , the peak of the each pulse is reduced. Consequently, a damage on the wafer  1  can be prevented from being caused.  
         [0064]     In addition, when a configuration described with reference to  FIGS. 9-11  is adopted as the irradiation optical system  152  and the detection optical system  153 , it becomes possible to discriminate a kind and sizes of a detected defect by comparing detected signals that correspond to the respective irradiation or detection in each of which a state of polarization, an irradiation angle, and a detection angle are different.  
         [0065]     The method for detecting defects on a wafer by applying a pulsed laser beam that is made into a linear shape and is composed of divided pulses on the wafer explained in this embodiment can also be applied to the case of detecting defects on the surface of a wafer that has not undergone formation of the pattern explained in the first embodiment. At this time, the pulsed laser beam being made into a linear shape is applied on the wafer  1  so that its longitudinal direction may coincide with a radial direction of the wafer  1 . An image of the wafer surface irradiated with this pulsed laser beam being made into a linear shape is formed by an imaging optical system and picked up by the CCD sensor in synchronization with rotation of the wafer  1 .  
         [0066]     The invention maybe embodied in other specific forms without departing from the spirit or essential characteristics thereof. The present embodiment is therefore to be considered in all respects as illustrative and not restrictive, the scope of the invention being indicated by the appended claims rather than by the foregoing description and all changes which come within the meaning and range of equivalency of the claims are therefore intended to be embraced therein.