Method and apparatus for charge distribution analysis

Electricity: measuring and testing – A material property using electrostatic phenomenon

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324457, 324 72, 177210EM, G01N 2760

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active

051874423

DESCRIPTION:

BRIEF SUMMARY
BACKGROUND OF THE INVENTION

The present invention is directed to a new apparatus and method of charge distribution analysis, or CDA, to measure surface and/or subsurface charge layers, the sign of dominant charge carriers, and their mobility in--as well as the dielectric constant of--insulating and semiconducting dielectric materials.
The existence of surface/subsurface charge layers has been theoretically predicted on the basis of fundamental thermodynamic laws, specifically for ionic insulators. For instance, discussions of such charge layers may be found in the following articles: K. Lehovec, J. Chem. Phys. 21, 1123 (1953); K. L. Kliewer and J. S. Koehler, Phys. Rev. 140A, 1226 (1965); and W. D. Kingery, J .Am. Ceram. Soc. 57, 1 (1974) and 57, 74 (1974). A discussion of oxide insulators with electronic defects is found in the article by B. V. King and F. Freund, Phys. Rev B29, 5814 (1984). The presence of such charge layers has been concluded from a variety of indirect observations such as the preferred segregation of certain aliovalent cations to surfaces and/or grain boundaries (Kingery 1974 articles cited above), the deflection of low energy electron or ion beams from surfaces, the energy dispersion of photoelectrons emitted from surfaces and many manifestations of electrostatic adhesion. Each of the above references is hereby incorporated herein by reference.
However, no method has existed until now for directly measuring and quantifying surface/subsurface charge layers, and for determining the sign and mobility of the dominant charge carriers.
Prior methods such as the measurement of cation surface or grain boundary segregation in ceramics are indirect and limited to high temperatures. They require thermal pretreatment of the samples, extensive sample preparation for observation of frozen-in disequilibrium states by microanalytical techniques (Kingery 1974) or extremely clean surface conditions in ultrahigh vacuum. Prior methods such as the deflection or energy dispersion of low energy charged beams, both electrons and other particles, inherently require high or ultrahigh vacua, and are restricted to very thin surface/subsurface layers due to the limited depth of penetration or escape depth of low energy electron or ion beams.
Prior methods such as based on electrostatic adhesion are qualitative at best, giving no or very limited information about the strength of the effect, about the concentration and the nature of the dominant charge carriers.


SUMMARY OF THE INVENTION

It is an object of this invention to provide a method for charge distribution analysis, or CDA, for measuring surface/subsurface charge layers, and for determining the sign of the dominant charge carriers and their mobility in insulating and semiconducting dielectric materials.
It is a further object of this invention to utilize as a force sensor an electronic force-sensitive device or a balance, appropriately called a Coulomb Balance, to measure the force between a dielectric material carrying a surface/subsurface charge layer and a bias electrode at close proximity to which a voltage may be applied.
It is still another object of this invention to measure this force as a function of various physical parameters including, but not limited to, the sign of the applied voltage, the magnitude of the applied voltage, sample position, sample temperature, photon flux, phonon (sound wave) flux, electron bombardment and particle bombardment.
It is a further object of this invention to provide a method for measuring the magnetic susceptibilities of materials independent of mass losses or mass gains of these materials during measurement.
It is a further object of this invention to provide a method for measuring simultaneously, within the same apparatus, dielectric and magnetic susceptibilities and derivative properties of materials independent of mass losses or mass gains during measurement.
It is a further object of this invention to utilize a vertical pendulum with its axis z set parallel to the prevailing gravitational vector g, with for

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Lehovec, (1953) J. Chem. Phys. 21(7):1123-1128.
Kliewer et al., (1965) Phys. Rev. 140(4A):1226-1246.
Kingery, (1974) J. Am. Ceram. Soc. 57(2):74-83.
King et al., (1984) Physical Review B29(10):5814-5824.
Freund, (1985) Journal of Non-Crystalline Solids 71:195-202.
Product Descriptions in Performance Specifications (Apr. 1, 1988), pp. 1-11.
Perkin-Elmer Corporation, "Instructions for TGS-1 Thermobalance," 1967, pp. 1-1 through 8-1.

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