Fig. 3.

A full-scan solution of Eq. (14) that does not limit scan rates. RS signal may not decay by the end of a half-scan (a). Constant B₁ can be represented as a sum of up-scan (green) and down-scan (magenta) step-functions (b). Separation of m(t) in (a) into its corresponding excitations responses (c) and (d) permits the stable deconvolution described by Eq. (17).