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 |
|
| Publication status | Published - 2023 |
Fingerprint
Dive into the research topics of '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)'. Together they form a unique fingerprint.Research output
- 1 Article
-
Wave-field representations with Green's functions, propagator matrices, and Marchenko-type focusing functions
Wapenaar, C. P. A., 2022, In: The Journal of the Acoustical Society of America. 151, 1, p. 587-608 22 p.Research output: Contribution to journal › Article › Scientific › peer-review
Open AccessFile9 Link opens in a new tab Citations (Scopus)151 Downloads (Pure)
Cite this
- APA
- Author
- BIBTEX
- Harvard
- Standard
- RIS
- Vancouver