Simultaneous Observation of Enzyme Surface Diffusion and Surface Reaction Using Microfluidic Patterning of Substrate Surfaces

2005 ◽  
Vol 77 (24) ◽  
pp. 8146-8150 ◽  
Author(s):  
Shaunak Roy ◽  
Jerry M. Thomas ◽  
Elizabeth A. Holmes ◽  
James T. Kellis, ◽  
A. J. Poulose ◽  
...  
1991 ◽  
Vol 236 ◽  
Author(s):  
Mitsugu Hanabusa ◽  
Hideki Ouchi ◽  
Kenji Ishida ◽  
Masahiro Kawasaki ◽  
Satoshi Shogen

AbstractAluminum thin film was deposited via a photochemical surface reaction of dimethylaluminum hydride (DMAH) using a deuterium lamp. The period required to initiate the film growth differed with substrate, and making use of this result the film could be grown preferentially on silicon nitride and silicon oxide layers rather than on wet-etched silicon. On the basis of an x-ray photoelectron spectroscopy the observed dependence of photodeposition on substrate surfaces can be attributed to how DMAH is chemisorbed initially.


Author(s):  
Anirudh Udupa ◽  
Subramanya Sadasiva ◽  
Ganesh Subbarayan

Often during phase growth, the rate of accretion, on the one hand, is determined by a competition between bulk diffusion and surface reaction rate. The morphology of the phase interface, on the other hand, is determined by an interplay between surface diffusivity and surface reaction rate. In this study, a framework to predict the growth and the morphology of an interface by modelling the interplay between bulk diffusion, surface reaction rate and surface diffusion is developed. The framework is demonstrated using the example of Cu–Sn intermetallic compound growth that is of significance to modern microelectronic assemblies. In particular, the dynamics and stability of the interface created when Cu and Sn react to form the compound Cu 6 Sn 5 is explored. Prior experimental observations of the Cu 6 Sn 5 –Sn interface have shown it to possess either a scalloped, flat or needle-shaped morphology. Diffuse interface simulations are carried out to elucidate the mechanism behind the interface formation. The computational model accounts for the bulk diffusion of Cu through the intermetallic compound, reaction at the interface to form Cu 6 Sn 5 , surface diffusion of Cu 6 Sn 5 along the interface and the influence of the electric current density in accelerating the bulk diffusion of Cu. A stability analysis is performed to identify the conditions under which the interface evolves into a flat, scalloped or needle-shaped structure.


1989 ◽  
Vol 164 ◽  
Author(s):  
A. Matsuda ◽  
T. Goto

AbstractThe role of the surface reaction is discussed in the formation process of µc-Si:H in comparison to that of a-Si:H. It is suggested that the responsible radicals for the formation of µc-Si:H are SiH3 as same in the case of a-Si:H depositions. On the top film-growing surface, a lot of H atoms reach the surface during the course of the μc-Si:H growth giving rise to the change in the surface condition, i. e. the loss probability of SiH3 radicals is increased. At the same time, a full H-coverage of the surface is expected which enhances the surface diffusion of SiH3 radicals, leading to the appearance of a gc nucleus. Moreover, it is speculated that the reaction in the growth zone is not necessary for the nucleation process in µc-Si:H.


Author(s):  
J.T. Fourie

Contamination in electron microscopes can be a serious problem in STEM or in situations where a number of high resolution micrographs are required of the same area in TEM. In modern instruments the environment around the specimen can be made free of the hydrocarbon molecules, which are responsible for contamination, by means of either ultra-high vacuum or cryo-pumping techniques. However, these techniques are not effective against hydrocarbon molecules adsorbed on the specimen surface before or during its introduction into the microscope. The present paper is concerned with a theory of how certain physical parameters can influence the surface diffusion of these adsorbed molecules into the electron beam where they are deposited in the form of long chain carbon compounds by interaction with the primary electrons.


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