Emergence of the stripe-domain phase in patterned permalloy films

被引:26
|
作者
Voltan, S. [1 ]
Cirillo, C. [2 ,3 ]
Snijders, H. J. [1 ]
Lahabi, K. [1 ]
Garcia-Santiago, A. [4 ,5 ]
Hernandez, J. M. [4 ,5 ]
Attanasio, C. [2 ,3 ]
Aarts, J. [1 ]
机构
[1] Leiden Univ, Kamerlingh Onnes Huygens Lab, POB 9504, NL-2300 RA Leiden, Netherlands
[2] Univ Salerno, CNR SPIN Salerno, Via Giovanni Paolo 2 132, I-84084 Fisciano, Sa, Italy
[3] Univ Salerno, Dipartimento Fis ER Caianiello, Via Giovanni Paolo 2 132, I-84084 Fisciano, Sa, Italy
[4] Univ Barcelona, Grp Magnetisme, Dept Fis Fondamental, Fac Fis, C Marti & Franques 1,Planta 4,Edifici Nou, E-08028 Barcelona, Spain
[5] Univ Barcelona, Inst Nanociencia & Nanotecnol IN2UB, C Marti & Franques 1,Planta 3,Edifici Nou, E-08028 Barcelona, Spain
关键词
FERROMAGNETIC-RESONANCE;
D O I
10.1103/PhysRevB.94.094406
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
The occurrence of stripe domains in ferromagnetic permalloy (Py = Fe20Ni80) 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-domain (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-domain (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.
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页数:8
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