Effects of A-site cationic radius and cationic disorder on the electromagnetic properties of La0.7Ca0.3MnO3 ceramic with added Sr, Pb, and Ba

2018 ◽  
Vol 44 (5) ◽  
pp. 5378-5384 ◽  
Author(s):  
Yule Li ◽  
Hui Zhang ◽  
Qingming Chen ◽  
Di Li ◽  
Zhiyu Li ◽  
...  
2020 ◽  
Vol 31 (10) ◽  
pp. 7623-7629
Author(s):  
Fuxin Ling ◽  
Di Li ◽  
Ling Li ◽  
Hui Zhang ◽  
Ping Yu ◽  
...  
Keyword(s):  
Sol Gel ◽  

1990 ◽  
Vol 95 (4) ◽  
pp. 679-696 ◽  
Author(s):  
J B Lansman

Currents flowing through single dihydropyridine-sensitive Ca2+ channels were recorded from cell-attached patches on C2 myotubes. In the presence of dihydropyridine agonist to prolong the duration of single-channel openings, adding micromolar concentrations of lanthanum (La), cerium (Ce), neodymium (Nd), gadolinium (Gd), dysprosium (Dy), or ytterbium (Yb) to patch electrodes containing 110 mM BaCl2 caused the unitary Ba2+ currents to fluctuate between fully open and shut states. The kinetics of channel blockade followed the predictions of a simple open channel block model in which the fluctuations of the single-channel current arose from the entry and exit of blocking ions from the pore. Entry rates for all the lanthanides tested were relatively insensitive to membrane potential, however, exit rates depended strongly on membrane potential increasing approximately e-fold per 23 mV with hyperpolarization. Individual lanthanide ions differed in both the absolute rates of ion entry and exit: entry rates decreased as cationic radius decreased; exit rates also decreased with cationic radius during the first part of the lanthanide series but then showed little change during the latter part of the series. Overall, the results support the idea that smaller ions enter the channel more slowly, presumably because they dehydrate more slowly; smaller ions also bind more tightly to a site within the channel pore, but lanthanide residence time within the channel approaches a maximum for the smaller cations with radii less than or equal to that of Ca2+.


2017 ◽  
Vol 442 ◽  
pp. 196-199 ◽  
Author(s):  
Suvayan Saha ◽  
Kalipada Das ◽  
Sudipta Bandyopadhyay ◽  
I. Das
Keyword(s):  
A Site ◽  

2016 ◽  
Vol 80 (2) ◽  
pp. 474-479 ◽  
Author(s):  
Xiaohui Chen ◽  
Qingming Chen ◽  
Fei Jin ◽  
Xiang Liu ◽  
Hui Zhang

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.


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