Abstract
The mathematical modelling of ‘NMR imaging’ is presented from the electrical system design viewpoint. The response, namely, the magnetisationMxy(t), is linearly related to a system identification function made up of the nuclear spin density distribution ρ(r) and the relaxation times T1(r) and T2(r), while the r.f. excitation affects the system nonlinearly and appears as an ‘aperture’ function in the imaging equation.
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