2004
DOI: 10.1103/physrevb.70.094408
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Selective surface/interface characterization of thin garnet films by magnetization-induced second-harmonic generation

Abstract: Magnetization~induced second-harmonic generation (SHG) has been used for the study of thin garnet films. The strong optical absorption of these films at the second harmonic frequency provides a unique possibility to study magnetic and structural properties of the film surface and film/substrate interface separately. When studied in transmission at normal incidence all relevant elements of the crystallographic part of the nonlinear optical susceptibility tensor vanish identically, while a magnetization· induced… Show more

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Cited by 19 publications
(13 citation statements)
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“…While bulk garnet crystals have cubic symmetry and possess a center of inversion, epitaxially grown thin garnet films seem to lack this center of symmetry, as has been demonstrated by the existence of a linear magnetoelectric effect 49 and by strong optical second-harmonic generation. 50,51 The garnet films were studied in transmission using an all-optical pump and probe technique. Regeneratively amplified 100 fs pulses of wavelength = 805 nm emitted from a Ti:Sapphire laser system at a repetition rate of 1 kHz were split into two parts using a beam splitter.…”
Section: Methodsmentioning
confidence: 99%
“…While bulk garnet crystals have cubic symmetry and possess a center of inversion, epitaxially grown thin garnet films seem to lack this center of symmetry, as has been demonstrated by the existence of a linear magnetoelectric effect 49 and by strong optical second-harmonic generation. 50,51 The garnet films were studied in transmission using an all-optical pump and probe technique. Regeneratively amplified 100 fs pulses of wavelength = 805 nm emitted from a Ti:Sapphire laser system at a repetition rate of 1 kHz were split into two parts using a beam splitter.…”
Section: Methodsmentioning
confidence: 99%
“…The sample was grown on a (001) oriented gadolinium gallium garnet substrate with trace amounts of Pb impurities resulting from the growth process. This sample has a magnetisation of M s = 300 kA m −1 [37] and a weak in-plane fourfold anisotropy field 4 kA m −1 which results, in the absence of magnetic fields, in four equilibrium orientations of the magnetisation that are orthogonal to each other in the plane of the film.…”
Section: Methodsmentioning
confidence: 99%
“…The quantitative values of the elements of the coupling tensor Γ αβγ have been chosen based on the values for the susceptibility χ αβγ experimentally determined and reported in [58]. Although, the exact numerical values with corresponding units could not be deduced from [58], we adopted the relations between the different tensor components mentioned in this article. In the present model the tensor components Σ α always occur in product with the saturation magnetization M s .…”
Section: Model Parametersmentioning
confidence: 99%