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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

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