scholarly journals Theory of half-metallic double perovskites. II. Effective spin Hamiltonian and disorder effects

2013 ◽  
Vol 87 (16) ◽  
Author(s):  
Onur Erten ◽  
O. Nganba Meetei ◽  
Anamitra Mukherjee ◽  
Mohit Randeria ◽  
Nandini Trivedi ◽  
...  
2004 ◽  
Vol 70 (18) ◽  
Author(s):  
R. Vidya ◽  
P. Ravindran ◽  
A. Kjekshus ◽  
H. Fjellvåg

2016 ◽  
Vol 30 (03) ◽  
pp. 1550260 ◽  
Author(s):  
I. Grusha ◽  
M. Menteshashvili ◽  
G. I. Japaridze

We derive an effective spin Hamiltonian for the one-dimensional half-filled asymmetric ionic Hubbard model (IHM) with alternating on-site interaction in the limit of strong repulsion. It is shown that the effective Hamiltonian is that of a spin S = 1/2 anisotropic XXZ Heisenberg chain with alternating next-nearest-neighbor (NNN) and three-spin couplings in the presence of a uniform and a staggered magnetic field.


2014 ◽  
Vol 75 ◽  
pp. 01001 ◽  
Author(s):  
B. Fisher ◽  
J. Genossar ◽  
K. B. Chashka ◽  
L. Patlagan ◽  
G. M. Reisner

2003 ◽  
Vol 68 (10) ◽  
Author(s):  
Z. Szotek ◽  
W. M. Temmerman ◽  
A. Svane ◽  
L. Petit ◽  
H. Winter

2022 ◽  
Vol 896 ◽  
pp. 163130
Author(s):  
Qasim Mahmood ◽  
Ghazanfar Nazir ◽  
Sonia Bouzgarrou ◽  
M.S. Rashid ◽  
Eman Algrafy ◽  
...  

2019 ◽  
Vol 5 (1) ◽  
Author(s):  
Jian Xu ◽  
Changsong Xu ◽  
Jian-Bo Liu ◽  
Laurent Bellaiche ◽  
Hongjun Xiang ◽  
...  

AbstractHalf-metallic ferromagnets (HMFs) that possess intriguing physical properties with completely spin-polarized current are key candidates for high-efficiency spintronic devices. However, HMFs that could simultaneously have high Curie temperature (Tc), wide half-metallic gap (ΔHM), and large bulk magnetocrystalline anisotropy energy (MAE) are very rare, which significantly restrict their room-temperature (RT) applications. In this article, through materials screening in layered halide double perovskites (LHDPs), we have theoretically identified that Cs4FePb2Cl12, which has good crystallographic, dynamic and thermal stabilities, possesses an intrinsic half-metallic ground-state with a high Tc ~ 450 K. Interestingly, the long-range ferromagnetic ordering in bulk Cs4FePb2Cl12 is contributed by the strong super-superexchange interactions between the neighboring Fe d orbitals mediated by different anionic Cl p orbitals. The high Tc of layered Cs4FePb2Cl12 can be well maintained even in the monolayer limitation, i.e., Tc ~ 370 K for Cs4FePb2Cl12 monolayer, which is critical for nanoscale device applications. Moreover, both bulk and monolayer Cs4FePb2Cl12 can exhibit wide ΔHM ~ 0.55 eV and large MAE >320 μeV/Fe, comparable to that of the best HMFs reported in the literature. Our findings can significantly extend the potentials of LHDPs for high-temperature spintronic applications.


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