scholarly journals Studying the Formation Process of Clusters in Solution at the Initial Stage of Protein Crystallization

Author(s):  
Bing Xiong ◽  
Guoliang Dai ◽  
Weihuo Li
Author(s):  
Y. yokota ◽  
H. Hashimoto

The initial stage of the reaction process forming the platinum silicide at Pt/Si (111) interfaces have been investigated by a high resolution electron microscope in both “flat-on” [1] and “cross-sectional” mode.First, platinum of 11 nm thickness was deposited on a Si (111) wafer. For observing the specimen in “flat-on” mode, the top surface and edge of the specimen were covered by paraffin and etched chemically using CP-4 reagent from backside. The specimen for observing in “cross-sectional” mode was prepared as follows. The Si wafer was cut into slips of 3mm width. After stacking 4 to 6 slips together with epoxy resin, the stacks were sliced to a thickness of 0.3-0.4mm by a diamond saw. The slices were mechanically polished to a thickness lower than 0.05mm and then thinned by Ar ion beam.The formation process of platinum silicide (PtSi) was observed in a cross-sectional specimen.


2009 ◽  
Vol 14 (8) ◽  
pp. 1377-1382 ◽  
Author(s):  
Na Wang ◽  
Wendi Zhang ◽  
Jipeng Xu ◽  
Bin Ma ◽  
Zongzhi Zhang ◽  
...  

2018 ◽  
Vol 175 ◽  
pp. 54-63 ◽  
Author(s):  
Shuai Wang ◽  
Yufeng Guo ◽  
Jianjun Fan ◽  
Yu He ◽  
Tao Jiang ◽  
...  

2010 ◽  
Vol 18 (3) ◽  
pp. 2090 ◽  
Author(s):  
M. Bello-Jiménez ◽  
E. A. Kuzin ◽  
O. Pottiez ◽  
B. Ibarra-Escamilla ◽  
A. Flores-Rosas ◽  
...  

2007 ◽  
Vol 561-565 ◽  
pp. 1703-1706 ◽  
Author(s):  
Ryusuke Nakamura ◽  
Daisuke Tokozakura ◽  
Jung Goo Lee ◽  
Hirotaro Mori ◽  
Hideo Nakajima

Oxidation behavior of Cu nanoparticles in the formation process of hollow Cu2O spheres was investigated by TEM. The thickness of Cu2O layers on Cu nanoparticles oxidized at 323 K in air was measured as a function of oxidation time. At the initial stage of oxidation until the oxide film with 2.5 nm in thickness is formed, the thickness of oxide films on Cu nanoparticles with the diameter of 10, 20 and 35 nm shows a nearly equal value regardless of diameter of Cu. After the formation of 2.5 nm layer, however, the growth rate of the oxide films on smaller nanoparticles becomes slower than that on larger nanoparticles. This result suggests that the voids formed at the Cu/Cu2O interface prevent Cu atoms from diffusing outward across the interface because the volume ratio of voids to inner Cu in smaller nanoparticles is much larger than that in larger nanoparticles.


2011 ◽  
Vol 20 (10) ◽  
pp. 1325-1328 ◽  
Author(s):  
Takahiro Maruyama ◽  
Satoshi Sakakibara ◽  
Shigeya Naritsuka ◽  
Kenta Amemiya

2021 ◽  
Author(s):  
Hiroki Okudera ◽  
Tetsuyoshi Takeda

Abstract It has been well known that a sedimentary precious opal is composed of closely packed uni-size silica spheres with voids filled by an air or water, and that an interference among reflections from the boundaries of those spheres and filler yields play-of-colour (iridescence). So, occurrence of a play-of-colour means occurrence of natural selection in size of spheres, or suppression of further nucleation after initial outburst of spheres, during its formation process. We had been exploring the possibility if we can regard a Stöber process as an analogue of the formation process of precious opal. The key is the reason why variation in size is rarely found on both precious opal and Stöber colloid. To give a clue, we examined the internal structure of Stöber particles and how those particles were formed at very initial stage of the process. The answers for evenness in shape and size are a quick supersaturation of reactive silica species, consecutive formation of large and loose polymers by fast dehydration, and their quick aggregation as the initial burst of silica spheres in highly diffusive medium. These can be achieved in nature by quick but continuous decrease in temperature on “basic” (high pH) geothermal hot water moving upward through cracks in rocks. Sedimentary precious opal can thus be formed when such naturally occurring colloid is filtered by a permeable bed.


1992 ◽  
Vol 280 ◽  
Author(s):  
Yasushi Sasajima ◽  
Syubo Taya ◽  
Satoru Ozawa ◽  
Ryoichi Yamamoto

ABSTRACTThe initial stage of film formation process was studied by 2 dimensional (2D) Monte-Carlo (MC) simulation and 3D molecular dynamics (MD) simulation. The atomistic interaction was simple pair-wise Lcnnard-Joncs potential for the 2D MC study and embedded atom potential (EAM potential) for the 3D MD simulation. The 2D MC study has revealed the dependence of film growth mode on the potential parameters that correspond to atomic size and binding energy. More realistic MD simulation has been performed using EAM potential for the three kinds of systems, Ni/Cu(111), Ag/Cu(111) and Au/Ni(111). The relaxed atomic structures of such systems showed the difference of atomic combination; coherent interface was obtained for Ni/Cu(111) system, incoherent interface with specific rotational relationships for Ag/Cu(111) andAu/Ni(111).


Sign in / Sign up

Export Citation Format

Share Document