Calcium Oxalate Nucleation and Growth on Oxide Surfaces

Author(s):  
Lin Song ◽  
Bruce C. Bunker ◽  
Gordon L. Graff ◽  
Michael J. Pattillo ◽  
Allison A. Campbell
1994 ◽  
Vol 346 ◽  
Author(s):  
Lin Song ◽  
Michael J. Pattillo ◽  
Gordon L. Graff ◽  
Allison A. Campbell ◽  
Bruce C. Bunker

ABSTRACTThe aqueous deposition of calcium oxalate onto colloidal oxides has been studied as a model system for understanding heterogeneous nucleation processes of importance in biomimetic synthesis of ceramic thin films. Calcium oxalate nucleation has been monitored by measuring induction times for nucleation using Constant Composition techniques and by measuring nucleation densities on extended oxide surfaces using an atomic force microscope. Results show that the dependence of calcium oxalate nucleation on solution supersaturation fits the functional form predicted by classical nucleation theories. Anionic surfaces appear to promote nucleation better than cationic surfaces, lowering the effective energy barrier to heterogeneous nucleation.


2019 ◽  
Vol 3 (15) ◽  
pp. 271-278 ◽  
Author(s):  
J. W. Elam ◽  
A. V. V. Zinovev ◽  
Michael J. Pellin ◽  
David J. Comstock ◽  
Mark C. Hersam

2020 ◽  
Vol 22 (36) ◽  
pp. 20515-20523
Author(s):  
Ryutaro Souda ◽  
Takashi Aizawa ◽  
Naoyuki Sugiyama ◽  
Masaki Takeguchi

Weakly chemisorbed water species on oxide surfaces inhibit epitaxial ice growth because they hamper the orientation flexibility of molecules for nucleation commensurate with the substrate.


2001 ◽  
Vol 672 ◽  
Author(s):  
S. M. George ◽  
J.W. Elam ◽  
R.K. Grubbs ◽  
C.E. Nelson

ABSTRACTNucleation and growth has been studied during tungsten (W) atomic layer deposition (ALD) on oxide surfaces. Auger electron spectroscopy (AES) was utilized to examine the deposition of W during the sequential (A) WF6 and (B) Si2H6 reaction cycles that define W ALD. The AES results displayed an initial nucleation period of ∼10 AB cycles to deposit one tungsten monolayer on SiO2. Subsequently, the W and Si AES signals grew and oscillated dramatically versus WF6 and Si2H6 exposures. The increase in the W AES signal in the growth region was consistent with a W ALD growth rate of 3.5 Å per AB cycle. An examination of the oxygen and tungsten AES signals versus AB cycles indicated that W ALD displayed nearly ideal “layer-by-layer”, Frank- van der Merwe growth after the nucleation period. On Al2O3, the AES results displayed a much shorter nucleation period for W ALD. Only 3 AB cycles were required to deposit one tungsten monolayer. Subsequently, the tungsten film grew at a rate of 3.6 Å per AB cycle. The initial nucleation period and growth mechanism during ALD are important because they will affect the roughness of the resulting ALD film.


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