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Surface diffraction on magnetic nanostructures in thin films using grazing incidence SANS. M. Pannetier (a), F. Ott (b), C. Fermon (b), Y. Samson (c) (a)

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Presentation on theme: "Surface diffraction on magnetic nanostructures in thin films using grazing incidence SANS. M. Pannetier (a), F. Ott (b), C. Fermon (b), Y. Samson (c) (a)"— Presentation transcript:

1 Surface diffraction on magnetic nanostructures in thin films using grazing incidence SANS. M. Pannetier (a), F. Ott (b), C. Fermon (b), Y. Samson (c) (a) DRECAM/SPEC, CEA Saclay, 91191 Gif sur Yvette FRANCE (b) Lab. Léon Brillouin CEA/CNRS, 91191 Gif sur Yvette FRANCE (c) CEA Grenoble DRFMC/SP2M, 17 rue des Martyrs 38054 Grenoble France

2 Outline Principle of the experiment Scattering on a FePd system Data simulations Other prospective systems

3 Principle of the experiment Under total reflection angle ( c ) an evanescent wave is travelling parallel to the surface penetration depth 10-50 nm i < c kiki kfkf

4 Scattering geometry z xy neutrons Incidence plane 10 -4 < Q y < 10 -2 nm -1 600 nm < < 60 µm incidence plane 10 -2 < Q y < 3 nm -1 10 -1 nm < < 100 nm

5 Experimental set-up Spectrometer PAPOL at the LLB Saclay sample slit 1H Specular reflected beam Incidence angle on the sample i slit 2H diffracted beam polariser Detector Y X Z

6 FePd layers Fe 0.5 Pd 0.5 alloy layers self- organise in magnetic stripes Domain sizes :60 nm Wall thickness :6 nm Magnetic domains Field B = Hd + M Simulation OOMMF DRFMC CEA Grenoble

7 Magnetic sensitivity Top view kiki kfkf qyqy The domains magnetisation contribute to the scattering Neel caps do not contribute Bloch wall do contribute Néel cap Mup Mdo

8 M and B components in the layer MBMB X Y Z

9 GID scattering on the PSD c = 0.7° Beam stop diffraction Specular line Refracted signal Qy Qz

10 Calcul plus complet (facteur de forme inclus) Sin(PhiF) vs Sin(Theta out) ; Theta In = 0.2° (stupide) Gauche ligne sur substrat; droite vraie situation (sauf épaisseur) Les échelles de couleurs ne corespondne tpas du tout au meme intensités!!!

11 Problem of the stray fields The stray fields are not negligible – They create a rather large magnetic potential outside the layer

12 GID 2D grating (top view) TF Rods 2 /d d Ewald sphere kiki kfkf kiki

13 Other example : Co clusters in Al 2 O 3 Co/Al2O3 D.Babonneau et al, APL 76 (2000) 2 / 5.4nm GISANS Correlation fonction Form factor


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