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

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40 3. Experimental details<br />

a very good electron focusing is achieved, one can observe very sharp diffraction spots of<br />

only one order rather than elongated rods. Some inelastically scattered electrons penetrate<br />

the bulk crystal and can be detected besides the surface diffraction pattern. If they fulfill<br />

Bragg diffraction conditions in the bulk, they are observed as diagonal Kikuchi pattern connecting<br />

the intense surface diffraction points. 130 If there is no pattern at all or if it consists of<br />

concentric circles, the surface is not well ordered or even polycrystalline.<br />

Recording RHEED intensity oscillations of the specular reflex with time allows one to quantify<br />

the number of monolayers grown in MBE, if the Van-der-Merve growth mode is predominant,<br />

as illustrated in Fig. 3.4. The Oxide-MBE system at PGI-6 is equipped with a<br />

self-constructed RHEED system having a VARIAN 981 e-gun source in the main deposition<br />

chamber.<br />

3.2.2. Low-energy electron diffraction (LEED)<br />

camera<br />

LEED<br />

window<br />

screen<br />

incident beam<br />

Ewald sphere<br />

sample<br />

reciprocal<br />

rods<br />

electron gun<br />

spots<br />

4-grid LEED optics<br />

Figure 3.5.: LEED working principle.<br />

Low-energy electrons with energies from about 20 to 500 eV are ideal probes for surface<br />

studies, because they are mainly elastically scattered by atoms. According to the de Broglie<br />

relation, λ = √ 150.4/E0 e− ([λ] = Å, [E] = eV), typical LEED wavelengths are of the same magnitude<br />

as interatomic distances in crystals and comparable with that used in X-ray diffraction<br />

(see Sec. 3.4.2). The Ewald sphere intersects only the lattice rods at particular points that<br />

fulfill the Laue diffraction condition eq. (3.4), and the resulting LEED pattern consists of an<br />

ordered arrangement of spots. All surface diffraction patterns show a symmetry reflecting<br />

that of the crystal class and are centrally symmetric. The scale of the diffraction pattern<br />

depends on the electron energy and the size of the surface unit cell as<br />

√<br />

2π 2mE<br />

d ∝ 2 −|G ‖ | 2 , (3.5)<br />

where d is the real space lattice parameter, and G ‖ a reciprocal lattice vector in the surface<br />

plane. 79,131<br />

In the experimental work, a LEED image shall exhibit a sharp pattern and low background<br />

intensity. Defects and crystallographic imperfections will broaden spots and increase the

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