Jump to content

Cagniard–De Hoop method

From Wikipedia, the free encyclopedia
This is an old revision of this page, as edited by GreenC bot (talk | contribs) at 04:07, 13 February 2020 (Move 1 url. Wayback Medic 2.5). The present address (URL) is a permanent link to this revision, which may differ significantly from the current revision.

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.

Further reading