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Ab initio investigations of magnetic properties of ultrathin transition ...

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5.2 Results <strong>of</strong> Fe monolayer on different hexagonal substrates from non-collinear cal. 101<br />

in the hexagonal 2DIBZ. If the nearest neighbor interactions are weak, then higher order<br />

interactions will play a crucial role to stabilize the <strong>magnetic</strong> ground state <strong>of</strong> the system, and<br />

must not be ignored. This leads to a lifting <strong>of</strong> the degeneracy in Heisenberg model for linear<br />

combinations <strong>of</strong> two different spin spirals, Q 3ΓK/4 and Q MΓ/2 . Then we could calculate the<br />

higher order interactions from the total energy difference between Q and a superposition<br />

<strong>of</strong> ±Q. The superposition <strong>of</strong> ±Q is mapped to real space by 4 atoms per unit cell will<br />

double-RW-AFM order. Instead <strong>of</strong> the FM ground state from collinear calculations, we<br />

found that the higher order interactions do stabilize a collinear double-RW-AFM ground<br />

state constructed from Qs along the high symmetry line M-Γ for Fe monolayer on the<br />

Rh(111) substrate. We also studied Fe on Tc by performing non-collinear calculations and<br />

found that Fe monolayer has a 120 ◦ Néel ground state on Tc(0001), which is different from<br />

the RW-AFM ground state that would be predicted by collinear calculations using 2 atoms<br />

per unit cell.<br />

At the end <strong>of</strong> the chapter we compared our non-collinear results for Fe monolayer on 4d-<br />

TMs. Due to geometrical effects along the high symmetry line M-Γ, the strongly polarized<br />

4d substrate will break the degeneracy <strong>of</strong> the Q 3ΓK/4 and Q MΓ/2 in Heisenberg model. This<br />

lead us to modify the model Hamiltonian by adding a term which depends on the substrate<br />

Stoner parameter and the induced moments <strong>of</strong> the substrates.

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