Enhancement in A-B super-exchange interaction with Mn substitution in Mg-Zn ferrites as a heating source in hyperthermia applications

2017 ◽  
Vol 43 (16) ◽  
pp. 13661-13669 ◽  
Author(s):  
Rohit Sharma ◽  
Prashant Thakur ◽  
Manoj Kumar ◽  
P.B. Barman ◽  
Pankaj Sharma ◽  
...  
Small ◽  
2019 ◽  
Vol 15 (39) ◽  
pp. 1903120 ◽  
Author(s):  
Jie Dai ◽  
Yinlong Zhu ◽  
Yichun Yin ◽  
Hassan A. Tahini ◽  
Daqin Guan ◽  
...  

2014 ◽  
Vol 70 (a1) ◽  
pp. C620-C620
Author(s):  
Tri Nguyen Van

The modulated structure by high pressure and the superconductivity of YBCO compounds have been revealed over two decades [1]. However, their nature & mechanism are not yet sufficiently known. Continuing the achieved results [2-3], the present paper aims to evidence how the Quantum Electron-Magnetic Phenomenon, namely the Super-Exchange Interaction of the "active electrons", i.e. the hybridized odd electrons from the Cu ions in the Cu-Y-Cu nanolayer as a Nanowaveguide (NWG), conditions the Superconductivity of YBCO. The 1st key: The nanostructure is of Quantum nature. The active electrons behavior as the Quasi-Free Electrons (QFEs) waving in the Quantum Well (NWG), where they can be favored to a strong Super-Exchange Interaction. Thereby, two types of the spin coupled pairs can be spontaneously formed in the NWG, where just the singlet pairs will play the role of the superconducting Cooper pairs. For studying these nanoeffects, ESR can offer an especially efficacious contribution. The 2nd key: On the basis of the consequences of the Pauli principle, the singlet pair only persists if its QFE cloud overlapping path length L = nλ/2, where λ is the de Broglie wavelength of QFE conditioned by the Nanodimension of the NWG (Fig.1, left). This electron waving status corresponds to an ideal metallic phase occurring in the NWG. The 3rd key: The spin coupling brings about a temperature depending Spin Gap of the QFEs in the NWG. Just this Spin Gaps causes the superconductivity with the phase transition characteristics (Fig.1, right) that exactly and surprisingly correspond with the experimental.


2000 ◽  
Vol 516 (1) ◽  
pp. 43-47 ◽  
Author(s):  
A. Elmali ◽  
Y. Elerman ◽  
I. Svoboda ◽  
H. Fuess

2000 ◽  
Vol 623 ◽  
Author(s):  
K. Sato ◽  
H. Katayama-Yoshida ◽  
T. Yamamoto

AbstractWe propose a new valence control method of codoping with doping Ga (or In, Al) donor and N acceptor at the same time for the fabrication of a low-resistivity p-type ZnO based upon the ab initio calculation. We compare our predicted materials design to fabricate a low resistivity p-type ZnO with the recent successful codoping. Based upon the success in the valence control of ZnO, we propose a materials design to fabricate the ferromagnetic Mn-doped p-type ZnO upon codoping. It is shown that the anti-ferromagnetic state is more stable than the ferromagnetic ones due to the anti-ferromagnetic super-exchange interaction, if we have no mobile holes. Upon codoping with the mobile holes, it is shown that the ferromagnetic state becomes more stable than the anti-ferromagnetic ones due to the ferromagnetic double-exchange interaction. However, it is shown that the anti-ferromagnetic state is more stable upon electron doping due to the anti-ferromagnetic super-exchange interaction. We calculate the chemical trends of the magnetic state in V-, Cr-, Fe-, Co-, and Ni-doped (25 at%) in ZnO, and predict that all of these materials show the ferromagnetic ground states without electron and hole doping.


2021 ◽  
Vol 230 ◽  
pp. 117733
Author(s):  
H. Félix-Quintero ◽  
C. Falcony ◽  
L. Mariscal-Becerra ◽  
E.V. Mejía-Uriarte ◽  
J. Hernández A. ◽  
...  

2020 ◽  
Vol 56 (1) ◽  
pp. 581-591
Author(s):  
Heiddy P. Quiroz ◽  
E. F. Galíndez ◽  
A. Dussan ◽  
A. Cardona-Rodriguez ◽  
Juan Gabriel Ramirez

2018 ◽  
Vol 93 (2) ◽  
pp. 169-174 ◽  
Author(s):  
V. Jagadeesha Angadi ◽  
Shidaling Matteppanavar ◽  
N. Maramu ◽  
P. Mohan Kumar ◽  
U. Mahaboob Pasha ◽  
...  

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