1982
DOI: 10.1111/j.1365-246x.1982.tb06394.x
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Computation of wave fields in inhomogeneous media -- Gaussian beam approach

Abstract: An asymptotic procedure for the computation of wave fields in two-dimensional laterally inhomogeneous media is proposed. It is based on the simulation of the wave field by a system of Gaussian beams. Each beam is continued independently through an arbitrary inhomogeneous structure. The complete wave field at a receiver is then obtained as an integral superposition of all Gaussian beams arriving in some neighbourhood of the receiver. The corresponding integral formula is valid even in various singular regions w… Show more

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Cited by 508 publications
(206 citation statements)
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“…) is the windowed data The form of the beams can be taken as Gaussian beams (e.g., Cerveny, 1982). If the beam widths are infinite, then we have plane wave extrapolation such as the double-square-root operator, plane wave migration, offset plane waves etc.…”
Section: Methods and Theorymentioning
confidence: 99%
“…) is the windowed data The form of the beams can be taken as Gaussian beams (e.g., Cerveny, 1982). If the beam widths are infinite, then we have plane wave extrapolation such as the double-square-root operator, plane wave migration, offset plane waves etc.…”
Section: Methods and Theorymentioning
confidence: 99%
“…The accuracy of the beam off the central ray is determined by the truncation error of Taylor expansion, and the approximate solution is given by a sum of all the beams (see [4,13,25]). The accuracy of the Taylor expansion was studied by Motamed and Runborg [24], and Tanushev [30] developed and analyzed higher order Gaussian beams giving better accuracy of the approximations.…”
Section: )mentioning
confidence: 99%
“…(1) is comprised of a Gaussian distribution with a linear phase-term which causes the beam to tilt with respect to the z = 0 plane. The tilted GBs in [24] were obtained by introducing a novel non-orthogonal coordinate system which is a priori matched to distribution (1). In this system r b = (x b 1 , x b 2 , z b ) where the z b -axis is in the beam-axis propagation direction and the transverse coordinates, x b 1 and x b 2 , lie on a plane parallel to the (x 1 , x 2 ) plane and are centered at its intersection with the z b -axis (see Fig.…”
Section: Tilted Gaussian Beamsmentioning
confidence: 99%
“…This feature is significantly advantageous for propagation and scattering and results in simplified analytic expressions for the beam fields. Locality considerations have been utilized for solving beam-type waveobjects propagation in generic media profiles such as inhomogeneous [1][2][3], anisotropic [4][5][6][7][8][9][10][11], and for time-dependent pulsed beams, in dispersive media [12][13][14][15][16].…”
Section: Introductionmentioning
confidence: 99%