2019
DOI: 10.1109/tmag.2019.2935419
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Unstable Playback Response of CPP-GMR Read Head Induced by Electromagnetic Interference: Structural Dependence

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Cited by 4 publications
(5 citation statements)
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“…As shown in Figure 1 a, the sensing layers of the CPP-GMR read head targeted for AD of 1 Tb/in 2 are modelled, assuming that the head is sensing the magnetic stray field, H stray , of the medium. The reader width and stripe height of the head were set at 60 and 48 nm, respectively, since this dimension was claimed as the appropriate value for the CPP-GMR reader at an AD of 1 Tb/in 2 [ 30 ]. The combination of the CMFG electrodes and AgSn/InZnO spacer was performed due to their suitability for practical CPP-GMR devices [ 15 ].…”
Section: Cpp-gmr Modellingmentioning
confidence: 99%
“…As shown in Figure 1 a, the sensing layers of the CPP-GMR read head targeted for AD of 1 Tb/in 2 are modelled, assuming that the head is sensing the magnetic stray field, H stray , of the medium. The reader width and stripe height of the head were set at 60 and 48 nm, respectively, since this dimension was claimed as the appropriate value for the CPP-GMR reader at an AD of 1 Tb/in 2 [ 30 ]. The combination of the CMFG electrodes and AgSn/InZnO spacer was performed due to their suitability for practical CPP-GMR devices [ 15 ].…”
Section: Cpp-gmr Modellingmentioning
confidence: 99%
“…The aj = (Jħg())/(2eMs) is a spin torque factor where J is the polarized current density, ħ is the reduced Planck's constant, e is the electron charge value and  is the free layer thickness. The scalar function is given as g() = [-4+(1+p) 3 (3+cos)/4p 3/2 ] -1 , where  is the angle between the magnetizations of the free layer and the reference layer. A 2.5 × 2.5 × 2.5 nm 3 computational cell size and 0.1 ps time step were set for all cases of the simulations.…”
Section: A Modelling Of the Cpp-gmr Read Sensorsmentioning
confidence: 99%
“…On the other hand, an important finding was that the readback signal became more symmetric and less distorted at shorter SH and longer RW lengths. Higher distortion of signal from the head with longer SH and shorter RW lengths can be physically explained by the behavior of the demagnetization field, Hdemag, over the free layer region [3]. The Hdemag is theoretically a force pulling the magnetization toward the its opposite direction, which results in fluctuating magnetization dynamic causing higher instabilities.…”
Section: A Optimal Sizing Ot the Cpp-gmr Sensor For Ad Of 1 Tb/inmentioning
confidence: 99%
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“…The GMR effect was first observed in Fe/Cr multilayer structures by Fert et al and Grünberg et al in 1988 and soon became a popular research topic due to its great potential in the field of hard drives, memories, sensors, etc. [ 16 , 17 , 18 , 19 ]. In 1998, Baselt et al firstly reported the GMR-based biosensors [ 20 ].…”
Section: Introductionmentioning
confidence: 99%