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Starting from equation (9),
based on the Muir expansion for the square-root
Claerbout (1985),
we can write successively:
|  |
(19) |
| (20) |
| (21) |
If we make the notations
|  |
(22) |
we obtain the finite-differences solution to the
one-way wave equation in Riemannian coordinates:
|  |
(23) |
Next: Mixed domain
Up: Sava: Riemannian wavefield extrapolation
Previous: REFERENCES
Stanford Exploration Project
10/23/2004