Erratum: Wave-field representations with Green's functions, propagator matrices, and Marchenko-type focusing functions (J. Acoust. Soc. Am. (2022) 151 (587-608) DOI: 10.1121/10.0009236)

Kees Wapenaar

doi:10.1121/10.0020538

Erratum: Wave-field representations with Green's functions, propagator matrices, and Marchenko-type focusing functions (J. Acoust. Soc. Am. (2022) 151 (587-608) DOI: 10.1121/10.0009236)

Kees Wapenaar

Applied Geophysics and Petrophysics

Research output: Contribution to journal › Comment/Letter to the editor › Scientific › peer-review

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Abstract

For the elastodynamic wave equation discussed in Appendix A.4 in Ref. 1, the expressions for matrices ∼L 6 1 and ∼L 6 2 in Eqs. (A32) and (A33) must be multiplied by 61. In other words, the signs of ∼L _ ₁and ∼L _ ₂have to be changed, whereas the signs of ∼L 1 and ∼L 2 remain unchanged. With these corrections, matrix ∼L , defined in Eq. (A5), fulfills the symmetry property formulated by Eq. (A6). The corrections have no consequences for Eqs. (A36)-(A38).

Original language	English
Pages (from-to)	593
Number of pages	1
Journal	The Journal of the Acoustical Society of America
Volume	154
Issue number	2
DOIs	https://doi.org/10.1121/10.0020538
Publication status	Published - 2023

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Erratum: Wave-field representations with Green’s functions, propagator matrices, and Marchenko-type focusing functions [J. Acoust. Soc. Am. 151, 587–608 (2022)]Final published version, 645 KB

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abstract = "For the elastodynamic wave equation discussed in Appendix A.4 in Ref. 1, the expressions for matrices ∼L 6 1 and ∼L 6 2 in Eqs. (A32) and (A33) must be multiplied by 61. In other words, the signs of ∼L _ 1and ∼L _ 2have to be changed, whereas the signs of ∼L 1 and ∼L 2 remain unchanged. With these corrections, matrix ∼L , defined in Eq. (A5), fulfills the symmetry property formulated by Eq. (A6). The corrections have no consequences for Eqs. (A36)-(A38). ",

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Erratum: Wave-field representations with Green's functions, propagator matrices, and Marchenko-type focusing functions (J. Acoust. Soc. Am. (2022) 151 (587-608) DOI: 10.1121/10.0009236). / Wapenaar, Kees.
In: The Journal of the Acoustical Society of America, Vol. 154, No. 2, 2023, p. 593.

Research output: Contribution to journal › Comment/Letter to the editor › Scientific › peer-review

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T1 - Erratum

T2 - Wave-field representations with Green's functions, propagator matrices, and Marchenko-type focusing functions (J. Acoust. Soc. Am. (2022) 151 (587-608) DOI: 10.1121/10.0009236)

AU - Wapenaar, Kees

PY - 2023

Y1 - 2023

N2 - For the elastodynamic wave equation discussed in Appendix A.4 in Ref. 1, the expressions for matrices ∼L 6 1 and ∼L 6 2 in Eqs. (A32) and (A33) must be multiplied by 61. In other words, the signs of ∼L _ 1and ∼L _ 2have to be changed, whereas the signs of ∼L 1 and ∼L 2 remain unchanged. With these corrections, matrix ∼L , defined in Eq. (A5), fulfills the symmetry property formulated by Eq. (A6). The corrections have no consequences for Eqs. (A36)-(A38).

AB - For the elastodynamic wave equation discussed in Appendix A.4 in Ref. 1, the expressions for matrices ∼L 6 1 and ∼L 6 2 in Eqs. (A32) and (A33) must be multiplied by 61. In other words, the signs of ∼L _ 1and ∼L _ 2have to be changed, whereas the signs of ∼L 1 and ∼L 2 remain unchanged. With these corrections, matrix ∼L , defined in Eq. (A5), fulfills the symmetry property formulated by Eq. (A6). The corrections have no consequences for Eqs. (A36)-(A38).

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Erratum: Wave-field representations with Green's functions, propagator matrices, and Marchenko-type focusing functions (J. Acoust. Soc. Am. (2022) 151 (587-608) DOI: 10.1121/10.0009236)

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