Ab initio investigations of magnetic properties of ultrathin transition ...
Ab initio investigations of magnetic properties of ultrathin transition ...
Ab initio investigations of magnetic properties of ultrathin transition ...
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78 5 Fe monolayers on hexagonal non<strong>magnetic</strong> substrates<br />
monolayer. In our calculations we got a RW-AFM ground state with -114 meV/Fe atom,<br />
while in ref. [57] the same ground state but with -82 meV/Fe atom was obtained. This<br />
means that there is about 30 meV/Fe atom difference, which is very large if we have smaller<br />
energies (as we see in Rh, Ir cases in Fig. 5.3), where we are in the energy range <strong>of</strong> about<br />
30 meV/Fe atom. This will be discussed more in details in next section.<br />
E [meV/Fe]<br />
Δ<br />
200<br />
100<br />
−100<br />
−200<br />
Tc Ru Rh Pd<br />
2.66 μ Β<br />
hcp substrates fcc substrates<br />
0<br />
2.59 μ Β<br />
2.72 μ Β<br />
2.68 μ Β<br />
2.89 μ Β<br />
2.90 μ Β<br />
3.08 μ Β<br />
3.10 μ Β<br />
Re Os Ir Pt<br />
Figure 5.3: Total-energy difference between the FM (ΔE >0) and RW-AFM (ΔE