Cagniard–de Hoop method
In the mathematical modeling of seismic waves, the Cagniard–De Hoop method is a sophisticated mathematical tool for solving a large class of wave and diffusive problems in horizontally layered media. The method is based on the combination of a unilateral Laplace transformation with real and positive transform parameter and the slowness field representation. It is named after Louis Cagniard and Adrianus de Hoop; Cagniard published his method in 1939, and de Hoop published an improvement on it in 1960.
- De Hoop, A. T. "A modification of Cagniard's method for solving seismic pulse problems". Applied Scientific Research, B8 (1960): 349–356.
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