The narrowest feature on present-day integrated circuits is the gate oxide-
the thin dielectric layer that forms the basis of field-effect device struc
tures. Silicon dioxide is the dielectric of choice and, if present miniatur
ization trends continue, the projected oxide thickness by 2012 will be less
than one nanometre, or about five silicon atoms across(1). At least two of
those five atoms will be at the silicon-oxide interfaces, and so will have
very different electrical and optical properties from the desired bulk oxi
de, while constituting a significant fraction of the dielectric layer. Here
we use electron-energy-loss spectroscopy in a scanning transmission electr
on microscope to measure the chemical composition and electronic structure,
at the atomic scale, across gate oxides as thin as one nanometre. We are a
ble to resolve the interfacial states that result from the spillover of the
silicon conduction-band wavefunctions into the oxide. The spatial extent o
f these states places a fundamental limit of 0.7 nm (four silicon atoms acr
oss) on the thinnest: usable silicon dioxide gate dielectric. And for prese
nt-day oxide growth techniques, interface roughness will raise this limit t
o 1.2 nm.