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Inspection method and inspection system using charged particle beam



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Patent 6618850
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Document Number
US Patent 6618850
Issued Date
September 9, 2003
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Abstract
Secondary electrons and back scattered electrons generated by irradiating a wafer to be inspected, such as a semiconductor wafer, with a charged particle beam are detected by a detector. A signal proportional to the number of detected electrons is generated, and an inspection image is formed on the basis of this signal. On the other hand, in consideration of a current value and irradiation energy of a charged particle beam, an electric field on the surface of the inspection wafer, emission efficiency of the secondary electrons and back scattered electrons, and the like, an electric resistance and an electric capacitance are determined so as to coincide with those in the inspection image. In a state where a difference between a resistance value in a normal portion and a resistance value in a defective portion is sufficiently increased by using the charging generated by the irradiation of electron beams, an inspection is thereby conducted to detect a defect.
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Number of Claims:
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Owner
Hitachi, Ltd. (Tokyo,JP)
Published
September 9, 2003
Application Number
09/785,275
Filed
February 20, 2001
US Classification
716/20   716/19 716/21
Int'l Classification
G01R   31/311   (20060101)   G01R   31/28   (20060101)   H01J   37/28   (20060101)  
Examiner
Assistant Examiner
Priority Data
Feb 22, 2000 [JP] 2000-050501 Sep 07, 2000 [JP] 2000-276640
USPTO Field of Search
716/20   716/21   716/19  
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A charged particle beam apparatus for acquiring high-definition and highly contrasted observation images by detecting efficiently secondary signals without increasing aberration of the primary electron beam, detecting defects from observation images and thus increasing the inspection speed and enhancing the sensitivity of inspection. The desired area of the sample is scanned with a primary charged particle beam, and the secondary charged particles generated secondarily from the area by the irradiation of the primary charged particle beam are led to collide with the secondary electron conversing electrode, and then the secondary electrons generated by the first E.times.B deflector 31 arranged through an insulator on the surface of the secondary electron conversing electrode on the side of the sample is absorbed by the detector. At the same time, the deflection chromatic aberration that had been generated in the primary charged particle beam by the first E.times.B deflector is reduced by the second E.times.B deflector arranged on the first E.times.B deflector, to obtain high-definition and highly contrasted observation images free of shading.

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