CRUSTAL SEISMIC ANISOTROPY - SOME FIRST PRINCIPLES
While seismologists recognize that seismic anisotropy can originate from upper crustal fractures or by organized fine-scale layering of isotropic material, here we are most interested in crustal anisotropy produced by deformation during regional metamorphism. Fabric material anisotropy involves at least four factors that contribute to seismic anisotropy: (1) mineral CPO (crystal preferred orientation) and rock texture, (2) bulk representation and scales, (3) structural shape and internal geometries (e.g., "structural geometry" anisotropy), and (4) azimuthal behavior of the anisotropy and the necessity to not use the weak-anisotropy assumption. Recent laboratory measurements of rock velocities reveal that a "diagonal quasi-compressional wave measurement" or "VP-45o" effect can drastically alter the azimuthal behavior of seismic anisotropy in foliated crustal rocks.
Seismic anisotropy is best understood using the elastic stress-strain definition of wave propagation. Here, the earth media are represented by stiffness tensors. The anisotropic behavior of fabrics can be classified by their tensor symmetries (e.g., isotropic, hexagonal). In addition, tensor averaging methods allow us to examine the anisotropic response of larger scale structures occurring within metamorphic terranes which possess strong coherent internal structure. We review these factors that affect seismic anisotropy and identify topics that require further community investigations.