Abstract

Deviations of P‐wave reflection traveltimes from a hyperbola, called the nonhyperbolic or quartic moveout, need to be properly handled while processing the long‐spread seismic data. As observed nonhyperbolic moveout is usually attributed to the presence of anisotropy, we devote our paper to deriving and analyzing a general formula that describes azimuthally varying quartic moveout coefficient in a homogeneous, weakly anisotropic medium above a dipping, mildly curved reflector. Our result incorporates all known weak anisotropy approximations of the quartic moveout coefficient and extends them further to triclinic media. By comparing our approximation with nonhyperbolic moveout obtained from the ray‐traced reflection traveltimes, we find that the former satisfactory predicts azimuthal variations of the quartic moveout when its magnitude is less or about 20% of the corresponding hyperbolic moveout term. We also study the influence of reflector curvature on non‐hyperbolic moveout. It turns out that the curvature as such produces no quartic moveout in the reflector strike direction, where the anisotropy‐induced moveout nonhyperbolicity is usually non‐negligible. Thus, the presence of nonhyperbolic moveout along the reflector strike might serve as an indication of effective anisotropy.

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