Modeling the Interaction of the Phosphate Group in Nucleotides with Copper(I) in the Gas Phase:  Reactivity of Cu+with Orthophosphoric Acid and Its Monomethyl Ester

2000 ◽  
Vol 104 (1) ◽  
pp. 110-118 ◽  
Author(s):  
A. Luna ◽  
S. Gevrey ◽  
J. Tortajada
2019 ◽  
Vol 26 (1) ◽  
pp. 285-305
Author(s):  
Eva‐Maria Köck ◽  
Jürgen Bernard ◽  
Maren Podewitz ◽  
Dennis F. Dinu ◽  
Roland G. Huber ◽  
...  

2014 ◽  
Vol 126 (44) ◽  
pp. 11960-11965 ◽  
Author(s):  
Hans Peter Reisenauer ◽  
J. Philipp Wagner ◽  
Peter R. Schreiner

2014 ◽  
Vol 126 (44) ◽  
pp. 11853-11853
Author(s):  
Hans Peter Reisenauer ◽  
J. Philipp Wagner ◽  
Peter R. Schreiner

2014 ◽  
Vol 53 (44) ◽  
pp. 11667-11667 ◽  
Author(s):  
Hans Peter Reisenauer ◽  
J. Philipp Wagner ◽  
Peter R. Schreiner

2014 ◽  
Vol 53 (44) ◽  
pp. 11766-11771 ◽  
Author(s):  
Hans Peter Reisenauer ◽  
J. Philipp Wagner ◽  
Peter R. Schreiner

1998 ◽  
Vol 108 (6) ◽  
pp. 2458-2465 ◽  
Author(s):  
S. Gevrey ◽  
A. Luna ◽  
V. Haldys ◽  
J. Tortajada ◽  
J-P. Morizur

Author(s):  
Richard E. Hartman ◽  
Roberta S. Hartman ◽  
Peter L. Ramos

The action of water and the electron beam on organic specimens in the electron microscope results in the removal of oxidizable material (primarily hydrogen and carbon) by reactions similar to the water gas reaction .which has the form:The energy required to force the reaction to the right is supplied by the interaction of the electron beam with the specimen.The mass of water striking the specimen is given by:where u = gH2O/cm2 sec, PH2O = partial pressure of water in Torr, & T = absolute temperature of the gas phase. If it is assumed that mass is removed from the specimen by a reaction approximated by (1) and that the specimen is uniformly thinned by the reaction, then the thinning rate in A/ min iswhere x = thickness of the specimen in A, t = time in minutes, & E = efficiency (the fraction of the water striking the specimen which reacts with it).


Author(s):  
J.M. Guilemany ◽  
F. Peregrin

The shape memory effect (SME) shown by Cu-Al-Mn alloys stems from the thermoelastic martensitic transformation occuring between a β (L2,) metastable phase and a martensitic phase. The TEM study of both phases in single and polycrystalline Cu-Al-Mn alloys give us greater knowledge of the structure, order and defects.The alloys were obtained by vacuum melting of Cu, Al and Mn and single crystals were obtained from polycrystalline alloys using a modified Bridgman method. Four different alloys were used with (e/a) ranging from 1.41 to 1.46 . Two different heat treatments were used and the alloys also underwent thermal cycling throughout their characteristic temperature range -Ms, Mf, As, Af-. The specimens were cut using a low speed diamond saw and discs were mechanically thinned to 100 μm and then ion milled to perforation at 4 kV. Some thin foils were also prepared by twin-jet electropolishing, using a (1:10:50:50) urea: isopropyl alcohol: orthophosphoric acid: ethanol solution at 20°C. The foils were examinated on a TEM operated at 200 kV.


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