“…}\left( {\frac{1}{M}\mathop \sum \nolimits_{i = 1}^M \sqrt {{{\left( {{{\left( {\frac{{\partial G\left( {{x_i},\;{z_j}} \right)}}{{\partial x}}} \right)}^2} + {{\left( {\frac{{\partial G\left( {{x_i},\;{z_j}} \right)}}{{\partial z}}} \right)}^2}} \right)}^v}} }\right),\end{equation}$$in which i is the counter of observation data, j is the counter of interesting depth, M is the number of observations,
and
are the derivatives of
and v is called the degree of the NFG operator, which controls two important shaping parameters of an envelope, the peak value and the anomaly width of the NFG sections. Although v can be taken as 1, 2, 4, 8 and so forth, v = 1 is generally used for the potential field data (Aydin,
1997). Karsli (
2001) suggested that higher order values are more reasonable for seismic applications because they narrow the recorded signal's width and improve the seismic resolution.…”