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Magnetic Oxide Heterostructures: EuO on Cubic Oxides ... - JuSER

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2.3. Magnetic properties of EuO 15<br />

order to maintain the insulating nature of EuO tunnel contacts. An exotic method to provide<br />

itinerant 5d electrons in EuO 1−x is by light doping using a laser irradiation of hv ≈ 2eV. 23<br />

Finally, if chemical constituents with different ionic radii are incorporated into the crystal,<br />

this gives rise to isotropic strain (chemical pressure). This chemical pressure is supposed to<br />

vary the f –f and d–f exchange interactions. 69<br />

2.3.2. Thin film effects in EuO<br />

<br />

d EuO = 5.1 nm<br />

<br />

n=20<br />

<br />

z<br />

S<br />

d EuO = 2.6 nm<br />

4<br />

n=7<br />

3<br />

n=5<br />

2<br />

n=4<br />

1<br />

n=3<br />

n=2<br />

0<br />

n=1<br />

0 10 20 30 40 50 60 70<br />

Temperature (K)<br />

n=10<br />

n=15<br />

surface Layer<br />

center Layer<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

Figure 2.8.: Ferromagnetism in ultrathin EuO films. In (a), the Curie temperature is calculated by<br />

a ferromagnetic Kondo-lattice model and seen to be reduced with decreasing number of EuO<br />

monolayers. Adapted from Schiller and Nolting (2001). 70 Polycrystalline EuO thin films show<br />

a decrease in T C (b), that roughly matches the calculation depicted in (a). Adapted from Müller<br />

et al. (2009). 48<br />

Since we investigate mainly ultrathin EuO films (d 5 nm) in this thesis, the behavior of the<br />

magnetic moment and T C in dependence on the thickness is of fundamental interest. The<br />

ferromagnetism in fcc EuO depends on the inter-atomic exchange coupling of the 4f orbitals.<br />

This coupling will be affected by reduced dimensions, e. g. in ultrathin EuO films. Schiller<br />

and Nolting (2001) calculated the electronic structure of one up to 20 monolayers of singlecrystalline<br />

EuO as a function of temperature and thickness in a Kondo-lattice model. 70 In<br />

their study, the averaged spin moment of the 4f begins to reduce when the EuO thickness<br />

drops below 2.5 nm, as depicted in Fig. 2.8a. For one monolayer EuO, they found a T C of 15 K.<br />

Remarkably, the temperature-dependent magnetization curves of center layers follow a Brillouin<br />

function, while surface layers show a lower magnetization. This can be explained by the<br />

Heisenberg model: Eu 2+ ions in center layers can couple to 12 neighbors, while surface ions<br />

only to 8 nearest neighbors. Experimental evidence of the reduction of the Curie temperature<br />

is shown in Fig. 2.8b, where the T C values of polycrystalline EuO match Schiller’s model very

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