Quantitation of latent resist images using photon tunneling microscopy

Citation
Ja. Liddle et al., Quantitation of latent resist images using photon tunneling microscopy, J VAC SCI B, 16(6), 1998, pp. 3651-3654
Citations number
11
Categorie Soggetti
Apllied Physucs/Condensed Matter/Materiales Science","Material Science & Engineering
Journal title
JOURNAL OF VACUUM SCIENCE & TECHNOLOGY B
ISSN journal
10711023 → ACNP
Volume
16
Issue
6
Year of publication
1998
Pages
3651 - 3654
Database
ISI
SICI code
1071-1023(199811/12)16:6<3651:QOLRIU>2.0.ZU;2-2
Abstract
Photon tunneling microscopy (PTM) is an optical microscopy technique that c an, by using frustrated total internal reflection, be sensitive to changes in surface topography as small as 1 nm. We have developed a simple calibrat ion technique that generates plots of sample reflectivity as a function of topography. This empirical data is then used to convert a gray-scale image of a specimen into an accurate topographic image. Errors, such as accurate magnification calibration,and detector. nonlinearity, lead to only small di fferences between the empirical data and our theoretical prediction. We hav e used PTM to study the evolution of latent images in a chemically amplifie d resist, ARCH2, as a function of dose, both after exposure and after poste xposure bake, and have obtained good agreement between the topography measu red in the PTM with thickness changes determined by ellipsometry from large exposed areas. Comparison of the results of the PTM with those obtained by near-field scanning optical microscopy demonstrate that changes in topogra phy on the order of 3-5 nm are visible in the PTM. The topography that appe ars to develop in a latent image is a function of feature size. This effect occurs before the lateral resolution limit of the microscope is reached, a nd is a result of the mechanical constraint arising from unexposed resist m aterial around the exposed features. Techniques such as adjusting the polar ization and wavelength of the illumination can improve the sensitivity of t he technique to small changes in topography, while in the case of materials that undergo changes in refractive index, contrast can be seen even in the absence of topography. (C) 1998 American Vacuum Society. [S0734-211X(98)17 806-X].