The Use of Multiple Ion Exchange to Produce Energy Transfer in Beta Aluminas

1989 ◽  
Author(s):  
L. A. Momoda ◽  
J. D. Barrie ◽  
Bruce Dunn
Keyword(s):  
2012 ◽  
Vol 14 (8) ◽  
Author(s):  
Rustem Zairov ◽  
Asiya Mustafina ◽  
Nataliya Shamsutdinova ◽  
Mark H. Rümmeli ◽  
Rustem Amirov ◽  
...  

1993 ◽  
Vol 97 (33) ◽  
pp. 8650-8655 ◽  
Author(s):  
Elaine S. Brigham ◽  
Paul T. Snowden ◽  
Yeong Il Kim ◽  
Thomas E. Mallouk

Langmuir ◽  
2009 ◽  
Vol 25 (5) ◽  
pp. 3146-3151 ◽  
Author(s):  
Asiya R. Mustafina ◽  
Svetlana V. Fedorenko ◽  
Olga D. Konovalova ◽  
Anastasiya Yu. Menshikova ◽  
Nataliya N. Shevchenko ◽  
...  

2020 ◽  
Vol 22 (40) ◽  
pp. 23342-23350
Author(s):  
Dmitriy V. Marasanov ◽  
Leonid Yu. Mironov ◽  
Yevgeniy M. Sgibnev ◽  
Ilya E. Kolesnikov ◽  
Nikolay V. Nikonorov

Silver molecular clusters were synthesized in photo-thermo-refractive glasses using the Na+–Ag+ ion exchange technique followed by heat treatment.


2015 ◽  
Vol 51 (99) ◽  
pp. 17521-17524 ◽  
Author(s):  
Xiao-Li Hu ◽  
Chao Qin ◽  
Xin-Long Wang ◽  
Kui-Zhan Shao ◽  
Zhong-Min Su

A luminescent dye@MOFviaion-exchange of cationic dyes was used as a probe to sense explosives by tuning the energy transfer between two different emissions.


Author(s):  
Ann M. Thomas ◽  
Virginia Shemeley

Those samples which swell rapidly when exposed to water are, at best, difficult to section for transmission electron microscopy. Some materials literally burst out of the embedding block with the first pass by the knife, and even the most rapid cutting cycle produces sections of limited value. Many ion exchange resins swell in water; some undergo irreversible structural changes when dried. We developed our embedding procedure to handle this type of sample, but it should be applicable to many materials that present similar sectioning difficulties.The purpose of our embedding procedure is to build up a cross-linking network throughout the sample, while it is in a water swollen state. Our procedure was suggested to us by the work of Rosenberg, where he mentioned the formation of a tridimensional structure by the polymerization of the GMA biproduct, triglycol dimethacrylate.


Author(s):  
R.D. Leapman ◽  
P. Rez ◽  
D.F. Mayers

Microanalysis by EELS has been developing rapidly and though the general form of the spectrum is now understood there is a need to put the technique on a more quantitative basis (1,2). Certain aspects important for microanalysis include: (i) accurate determination of the partial cross sections, σx(α,ΔE) for core excitation when scattering lies inside collection angle a and energy range ΔE above the edge, (ii) behavior of the background intensity due to excitation of less strongly bound electrons, necessary for extrapolation beneath the signal of interest, (iii) departures from the simple hydrogenic K-edge seen in L and M losses, effecting σx and complicating microanalysis. Such problems might be approached empirically but here we describe how computation can elucidate the spectrum shape.The inelastic cross section differential with respect to energy transfer E and momentum transfer q for electrons of energy E0 and velocity v can be written as


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