A top surface imaging approach for the fabrication of submicron features on solid substrates has been developed. A monolayer film is exposed to patterned deep ultraviolet radiation, then selectively metallized using electroless deposition such that a thin metal layer (200-400 A) is deposited only in the unexposed areas. The film/metal assembly is a highly effective mask for reactive ion etching which can subsequently be stripped from the substrate after feature definition. Features with 0.3 t~m line width in polysilicon and working transistor test structures have been produced using this process.In considering the characteristics of an ideal imaging process for optical lithography, numerous factors must be taken into account (1). The well-known Rayleigh criterion [1] states that the minimum resolution or feature width (W) is directly proportional to the exposure wave length (X), a material specific k factor, and inversely proportional to the numerical aperture (NA) of the lensOptical lithography is progressing from g-line (436 nm) to i-line (365 nm) to deep UV (248 nm and 193 nm) exposure tools in order to meet the continuing demand for greater circuit density, which requires smaller feature sizes. A second measure of lithographic performance, the modulation transfer function (MTF), is maximized as both wavelength and imaging layer thickness decrease. However, the depth of focus (DOF) is also directly proportional to wavelength, as given in Eq.[2]Short wavelength sources and high NA lenses which are desirable for fine feature printing can result in DOFs that are too small to produce a focussed image in a typical 1.0-1.5 i~m thick photoresist.There are additional difficulties with changing to shorter wavelength. Many photoresists are highly absorbing below about 250 nm. Alternate resins have been developed based on a limited class of materials that have sufficient transparency in the deep ultraviolet (UV). In addition, standing wave effects are particularly serious with deep UV lithography because of the higher reflectivity of silicon at these wavelengths. The use of antireflection coatings to solve this problem adds to the complexity of the lithographic processing (2).In the above analysis, the laws of optical physics lead to the conclusion that optimal performance will be obtained by the use of short wavelength irradiation and ultra-thin imaging layers. With a deep UV sensitive top surface imaging (TSI) process, resolution and MTF are maximized. If the layer is sufficiently thin, resist transparency is not a problem and standing waves can not be supported. DOF is also not an issue, except that a planarizing layer is required for printing over topography.The photoresist systems currently under the most active investigation are the DNQ-novolaks (3), chemically amplified resists (4, 5), and silicon containing polymer systems (6, 7). With the latter, photooxidation throughout at least several hundred Angstroms of the resist produces an oxidized silicon material that is resistant to certain plasmas for pattern trans...