The in-plane rotation of weak magnetic stripe domains in ~100 nm thick Fe0.8Ga0.2 and Fe:N (Nitrogen implanted) films epitaxied on GaAs(001) was investigated combining magnetic force microscopy, vibration sample magnetometry, and x-ray resonant magnetic scattering measurements. These two systems are characterized by perpendicular energy density K_PMA of the order of 10^5 J/m^3 leading a quality parameter Q = K_PMA/(½ ?_0 M_s^2)< 1 and a consequent weak stripes regime (see Fig. 1). We analysed the behaviour of the stripe pattern under the application of a bias magnetic field along the in-plane direction perpendicular to the stripes, and made a comparison with the analogous behaviour at remanence (Fig.2). The experimental results have been explained by means of energy balance considerations.[1] Fields smaller than 400 Oe for Fe0.8Ga0.2 and 1000 Oe for Fe:N do not induce any stripe rotation. Interestingly, a deformation of the closure domains pattern was evidenced in Fe0.8Ga0.2 leading to a fully reversible magnetization motion. Larger fields produce a sudden rotation of the stripe structure. A phenomenological model is proposed to describe the origin of the critical field. [1] S. Fin et al. Phys. Rev. B 92, 224411 (2015)
Origin of the field threshold for in-plane rotation of weak magnetic stripe domains
MG Pini;A Rettori;S Tacchi;
2016
Abstract
The in-plane rotation of weak magnetic stripe domains in ~100 nm thick Fe0.8Ga0.2 and Fe:N (Nitrogen implanted) films epitaxied on GaAs(001) was investigated combining magnetic force microscopy, vibration sample magnetometry, and x-ray resonant magnetic scattering measurements. These two systems are characterized by perpendicular energy density K_PMA of the order of 10^5 J/m^3 leading a quality parameter Q = K_PMA/(½ ?_0 M_s^2)< 1 and a consequent weak stripes regime (see Fig. 1). We analysed the behaviour of the stripe pattern under the application of a bias magnetic field along the in-plane direction perpendicular to the stripes, and made a comparison with the analogous behaviour at remanence (Fig.2). The experimental results have been explained by means of energy balance considerations.[1] Fields smaller than 400 Oe for Fe0.8Ga0.2 and 1000 Oe for Fe:N do not induce any stripe rotation. Interestingly, a deformation of the closure domains pattern was evidenced in Fe0.8Ga0.2 leading to a fully reversible magnetization motion. Larger fields produce a sudden rotation of the stripe structure. A phenomenological model is proposed to describe the origin of the critical field. [1] S. Fin et al. Phys. Rev. B 92, 224411 (2015)File | Dimensione | Formato | |
---|---|---|---|
prod_358503-doc_117297.pdf
solo utenti autorizzati
Descrizione: Origin_of_the_field_threshold_for_in-plane_rotation_of_weak_magnetic_stripe_domains
Tipologia:
Versione Editoriale (PDF)
Licenza:
NON PUBBLICO - Accesso privato/ristretto
Dimensione
401.32 kB
Formato
Adobe PDF
|
401.32 kB | Adobe PDF | Visualizza/Apri Richiedi una copia |
I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.