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

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6.3 Co atomic chain on Rh(664): 109<br />

as on fcc(111) surface, in B-type step. These types <strong>of</strong> steps are called 〈001〉 or 〈111〉<br />

micr<strong>of</strong>aceted for A- and B-type, respectively. An example <strong>of</strong> B-type is a (p, p, p − 2)<br />

surface which consists <strong>of</strong> terraces with a width <strong>of</strong> p full atomic wires. For example, a Co<br />

wire on a B-type step edge can be modeled by Rh(111) surface which is cut in a way that<br />

produces Rh terraces with 6-atomic rows, i. e. a Rh(664) surface with each Rh-edge atom<br />

is replaced by Co, as illustrated in figure 6.5.<br />

Figure 6.5: A Rh(664) surface (S) atoms shown as gray spheres, the step-edge atoms are<br />

replaced by Co atoms represented as smaller red spheres. The three surface atoms that<br />

are nearest neighbors to the step-edge Co atom are indicated: in the upper terrace Su, the<br />

lower terrace Sl and in the direction <strong>of</strong> the bulk Sb. The angles θ and ϕ characterizing the<br />

direction <strong>of</strong> the spin-quantization axis are indicated with respect to the terrace normal.<br />

We performed calculations with ab <strong>initio</strong> full-potential linearized augmented plane wave<br />

(FLAPW) method, as implemented in the FLEUR code[50]. The calculations are based<br />

on GGA[69]. In our simulations <strong>of</strong> the Co atomic chain on Rh(664) surface, we used<br />

symmetric film geometry (Fig. 6.5) with 45 atoms per unit cell. We used the Rh in-plane<br />

lattice constant, 2.70 ˚A, and the six topmost interlayer distances were relaxed by force<br />

calculations. We used about 90 basis functions/atom with a muffin-tin radius <strong>of</strong> 1.22 ˚A<br />

for the Co chain atoms and 1.28 ˚A for the Rh atoms. The irreducible part <strong>of</strong> the surface<br />

Brillouin zone was sampled with 42 k� points.<br />

In table 6.1, we show the relaxation results <strong>of</strong> the Co atoms in a chain decorating the<br />

Rh(664) step edge calculated with respect to the ideal atom spacing in bulk Rh. From<br />

these results we notice that the Co relaxations with the upper terrace Rh atoms Co-Rhu<br />

are smaller by factor <strong>of</strong> one half than the similar Co-Rhl and Co-Rhb relaxations towards<br />

the lower atoms (c. f. fig.6.5). By that we expect a stronger Co hybridization with the<br />

lower terrace and the bulk Rh atoms. If we compare Co/Rh(664) relaxation results to what

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