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Micromagnetic modeling of spintronic devices: from uniform state to skyrmion

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Figura

Fig. 1.3: schematic representation of the creation of the spin-polarized current. Part of the  entering  spins  in  the  ferromagnet1  are  polarized  in  the  same  direction  of  M 1 ,  generating  the spin-polarized current, which will transfer a spin-t
Fig.  1.4:  (a)  schematic  illustration  of  the  spin-transfer  torque  exerted  on  the  free  layer  magnetization  in  an  OOP  device
Fig.  1.10:  the  Rashba  effect  arises  in  FM/HM  bilayers,  when  the  electrical  current  flows  through the ferromagnet
Fig.  2.1:  schematic  illustration  of  the  TMR  phenomenon  in  MTJs,  where  in  (a)  the  magnetization state is parallel, allowing many spin-UP electrons to tunnel from the pinned  layer to the free layer, in  (b) the magnetization state is  AP and j
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