2004
DOI: 10.1016/j.jmmm.2003.12.1068
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Boundary element method and micromagnetism coupling for magneto-resistive heads modeling

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Cited by 2 publications
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“…The most efficient computation technique is to express it as a convolution of the gradient Green function G , solution of the equation Δ G ( r − r ′)=− δ ( r − r ′) and the magnetic charges distribution inside the sensor ρ : Equation 5 Our approach was developed in two levels. The first one previously reported (Firastrau et al , 2004), called partial coupling, does not take into account the effects of the shields on the micromagnetic state of the sensor. In the equation (1), the ρ p factor denotes in this case only the media charges distribution along the cross‐track direction.…”
Section: Model Descriptionmentioning
confidence: 99%
“…The most efficient computation technique is to express it as a convolution of the gradient Green function G , solution of the equation Δ G ( r − r ′)=− δ ( r − r ′) and the magnetic charges distribution inside the sensor ρ : Equation 5 Our approach was developed in two levels. The first one previously reported (Firastrau et al , 2004), called partial coupling, does not take into account the effects of the shields on the micromagnetic state of the sensor. In the equation (1), the ρ p factor denotes in this case only the media charges distribution along the cross‐track direction.…”
Section: Model Descriptionmentioning
confidence: 99%