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1.
Sci Prog ; 87(Pt 4): 249-68, 2004.
Article in English | MEDLINE | ID: mdl-16028835

ABSTRACT

The charging effect of an insulating specimen from electron beam (e-beam) irradiation may be utilized to facilitate imaging in the scanning electron microscope (SEM). This has been confirmed by a great deal of experimental work during the last three decades. Particularly, recent investigations indicate that even located underneath insulating thin films that a low energy e-beam cannot penetrate, conductors not biased and overlay marks, are observable through a novel imaging pattern, charging contrast. Unlike conventional SEM contrasts, which usually reflect surface characteristics, the dynamic charging contrast can reveal information of underlying structures without any external exciting signal. The authors consider that this kind of charging contrast arises from the different redistribution rates of secondary electrons returning to the surface under the surface local field of the charged specimen. The charging contrast has the prospect of extending the SEM application and forming new testing methods matched with the fast development of integrated circuits.


Subject(s)
Biophysics/instrumentation , Image Processing, Computer-Assisted/methods , Microscopy, Electron, Scanning/instrumentation , Microscopy, Electron, Scanning/methods , Animals , Biophysics/methods , Electrons , Humans
2.
J Electron Microsc (Tokyo) ; 52(5): 455-8, 2003.
Article in English | MEDLINE | ID: mdl-14700076

ABSTRACT

A one-dimensional model is proposed for analysing static capacitance contrast (SCC) in scanning electron microscopy. For the large-scale integrated specimen covered by an insulating thin film, the imaging signal is calculated considering the redistribution of secondary electrons (SEs) and the charging process of the equivalent effective capacitance between the irradiation point and substrate. The calculated SCC as a function of the irradiation charge density is in good agreement with the experimental SCC. It is confirmed that the SCC arises from the redistribution of SEs and the difference in the effective capacitance of irradiation points under the condition of positive charging.

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