6533b854fe1ef96bd12adeee
RESEARCH PRODUCT
Emergence of the stripe-domain phase in patterned permalloy films
A. García-santiagoCarla CirilloJan AartsH.j. SnijdersS. VoltanCarmine AttanasioJoan Manel HernàndezKaveh Lahabisubject
PermalloyMaterials scienceMagnetoresistanceFerromagnetismeFOS: Physical sciences02 engineering and technology01 natural sciencesCondensed Matter::Materials ScienceSputteringPhase (matter)Mesoscale and Nanoscale Physics (cond-mat.mes-hall)0103 physical sciencesMagnetoresistènciaThin filmFilmsMagnetic domains010302 applied physicsCondensed Matter - Mesoscale and Nanoscale PhysicsCondensed matter physicsMagnetoresistanceCoercivity021001 nanoscience & nanotechnologyPermalloyMagnetic fieldFerromagnetismFerromagnetism0210 nano-technologyMagnetic domains; Permalloy; Filmsdescription
The occurrence of stripe domains in ferromagnetic Permalloy (Py=Fe$_{20}$Ni$_{80}$) is a well known phenomenon which has been extensively observed and characterized. This peculiar magnetic configuration appears only in films with a thickness above a critical value ($d_{cr}$), which is strongly determined by the sputtering conditions (i.e. deposition rate, temperature, magnetic field). So far, $d_{cr}$ has usually been presented as the boundary between the homogeneous (H) and stripe-domains (SD) regime, respectively below and above $d_{cr}$. In this work we study the transition from the H to the SD regime in thin films and microstructured bridges of Py with different thicknesses. We find there is an intermediate regime, over a quite significant thickness range below d$_{cr}$, which is signaled in confined structures by a quickly changing domain-wall configuration and by a broadening of the magnetoresistance dip at the coercive field. We call this the emerging stripe-domains (ESD) regime. The transition from the ESD to the SD regime is accompanied by a sharp increase of the magnetoresistance ratio at the thickness where stripes appear in MFM.
year | journal | country | edition | language |
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2016-09-06 |