scholarly journals A-site phase segregation in mixed cation perovskite

2021 ◽  
pp. 100064
Author(s):  
Lang Liu ◽  
Jiuzhou Lu ◽  
Hao Wang ◽  
Zhenhua Cui ◽  
Giacomo Giorgi ◽  
...  
2021 ◽  
Vol 6 (3) ◽  
pp. 837-847
Author(s):  
Pronoy Nandi ◽  
Zijia Li ◽  
Younghoon Kim ◽  
Tae Kyu Ahn ◽  
Nam-Gyu Park ◽  
...  
Keyword(s):  

MRS Advances ◽  
2020 ◽  
Vol 5 (1-2) ◽  
pp. 93-101
Author(s):  
L.R. Blackburn ◽  
S.K. Sun ◽  
L.J. Gardner ◽  
E.R. Maddrell ◽  
M.C. Stennett ◽  
...  

ABSTRACTImmobilisation of Pu in a zirconolite matrix (CaZrTi2O7) is a viable pathway to disposition. A-site substitution, in which Pu4+ is accommodated into the Ca2+ site in zirconolite, coupled with sufficient trivalent M3+/Ti4+ substitution (where M3+ = Fe, Al, Cr), has been systematically evaluated using Ce4+ as a structural analogue for Pu4+. A broadly similar phase assemblage of zirconolite-2M and minor perovskite was observed when targeting low levels of Ce incorporation. As the targeted Ce fraction was elevated, secondary phase formation was influenced by choice of M3+ species. Co-incorporation of Ce/Fe resulted in the stabilisation of a minor Ce-containing perovskite phase at high wasteloading, whereas considerable phase segregation was observed for Cr3+ incorporation. The most favourable substitution approach appeared to be achieved with the use of Al3+, as no perovskite or free CeO2 was observed. However, high temperature treatments of Al containing specimens resulted in the formation of a secondary Ce-containing hibonite phase.


2019 ◽  
Author(s):  
Dominik Kubicki ◽  
Daniel Prochowicz ◽  
Albert Hofstetter ◽  
Shaik Zakeeruddin ◽  
Michael Grätzel ◽  
...  

1998 ◽  
Vol 547 ◽  
Author(s):  
P.G. Radaelli ◽  
D.N. Argyriou ◽  
D.E. Cox ◽  
L. Capogna ◽  
H. Casalta ◽  
...  

AbstractThe structural, magnetic and transport phase diagrams of the manganese perovskites (general formula: A1-xA'xMnO3) are characterised by a variety of exotic phenomena, including high-temperature polaronic behaviour, charge, orbital and magnetic ordering and colossal magnetoresistance (CMR). These properties can be “tuned” by changing the doping level x, the electronic bandwidth (through the average A-site ionic radius, <rA>), and the A-site disorder, and are believed to be a manifestation of the underlying competition between electron-lattice coupling and double exchange. Usually, at low temperatures, one of these two interactions is dominant, resulting in a homogeneous ground state, which is either a metallic ferromagnet or a charge-ordered insulator. We have recently found, however, that, for special points in the phase diagram (x ~ 0.3,,<rA> ~ 1.18 Å), the competition can be preserved down to low temperatures, resulting in an inhomogeneous ground state at the microscopic level. This unusual state is characterised by the coexistence of charge-ordered and metallic domains, which are intertwined over a variety of length-scales, and appear to show spin-glass-like dynamics. Upon application of an external field (magnetic field, pressure or even x-rays), the domains grow to macroscopic sizes, resulting in phase segregation. We speculate that the evolution of the local magnetic and crystal structures during this phase segregation process may parallel those occurring, at much higher temperatures, for compounds displaying CMR behaviour at the paramagnetic-toferromagnetic transition. Very recently, it has been suggested that the charge-ordered state, which is stable for higher values of the Mn oxidation state (x ≥ 0.5), may also be associated with modulated mesoscopic phase segregation, in the form of “stripes”. This hypothesis will be discussed in the light of recent x-ray synchrotron and neutron diffraction data on the crystallographic and magnetic modulation in La0.33Ca0.67MnO3


2017 ◽  
Vol 139 (40) ◽  
pp. 14173-14180 ◽  
Author(s):  
Dominik J. Kubicki ◽  
Daniel Prochowicz ◽  
Albert Hofstetter ◽  
Shaik M. Zakeeruddin ◽  
Michael Grätzel ◽  
...  

Author(s):  
O.L. Krivanek ◽  
J. TaftØ

It is well known that a standing electron wavefield can be set up in a crystal such that its intensity peaks at the atomic sites or between the sites or in the case of more complex crystal, at one or another type of a site. The effect is usually referred to as channelling but this term is not entirely appropriate; by analogy with the more established particle channelling, electrons would have to be described as channelling either through the channels or through the channel walls, depending on the diffraction conditions.


Author(s):  
Fred Eiserling ◽  
A. H. Doermann ◽  
Linde Boehner

The control of form or shape inheritance can be approached by studying the morphogenesis of bacterial viruses. Shape variants of bacteriophage T4 with altered protein shell (capsid) size and nucleic acid (DNA) content have been found by electron microscopy, and a mutant (E920g in gene 66) controlling head size has been described. This mutant produces short-headed particles which contain 2/3 the normal DNA content and which are non-viable when only one particle infects a cell (Fig. 1).We report here the isolation of a new mutant (191c) which also appears to be in gene 66 but at a site distinct from E920g. The most striking phenotype of the mutant is the production of about 10% of the phage yield as “giant” virus particles, from 3 to 8 times longer than normal phage (Fig. 2).


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