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dc.contributor.authorPostava, Kamil
dc.contributor.authorYamaguchi, Tomuo
dc.date.accessioned2007-06-29T13:13:21Z
dc.date.available2007-06-29T13:13:21Z
dc.date.issued2001
dc.identifier.citationJournal of Applied Physics. 2001, vol. 89, issue 4, p. 2189-2193.en
dc.identifier.issn0021-8979
dc.identifier.issn1089-7550
dc.identifier.urihttp://hdl.handle.net/10084/60824
dc.language.isoenen
dc.publisherAmerican Institute of Physicsen
dc.relation.ispartofseriesJournal of Applied Physicsen
dc.relation.urihttp://dx.doi.org/10.1063/1.1344214en
dc.titleOptical functions of low-k materials for interlayer dielectricsen
dc.typearticleen
dc.identifier.locationNení ve fondu ÚKen
dc.description.abstract-enThe optical functions of low dielectric constant (low-k) materials have been determined using a high-precision four-zone null spectroscopic ellipsometer in the spectral range from 1.5 to 5.4 eV (230–840 nm wavelength region). The ellipsometric data were fitted simultaneously with near-normal incidence reflectivity spectra (ranging from 0.5 to 6.5 eV). A general method of simultaneous treatment of ellipsometric and reflectivity data is demonstrated on representative materials used in the semiconductor industry for interlayer dielectrics: (1) SiLK—organic dielectric resin from the Dow Chemical Company, (2) Nanoglass—nanoporous silica from the Honeywell Electronic Materials Company, and (3) tetra-ethyl-ortho-silicate (TEOS) (SiO2)—the standard dielectric material. The low-k materials (SiLK and Nanoglass) were prepared by a standard spin-coating process, while the SiO2 layer was prepared by thermal decomposition from TEOS onto single-crystal silicon wafers.en
dc.identifier.doi10.1063/1.1344214
dc.identifier.wos000166688300030


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