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Explicit solution of the inverse kinematic problem in the non-Herglotz case

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Abstract

The inverse kinematic problem is solved in the half space R ν+1+ ={(x,z)|z⩾0,x∈Rν, ν⩾1 under the assumption that the index of refraction can be represented in the form

$$n^2 (x,z) = K^2 (z) + \sum\limits_{j = 1}^\nu {\Phi _j^2 (x_j ),} n_z< 0.$$

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The solution obtained is a generalization of the Herglotz-Wiechert formula. A formula is presented for the solution of the inverse kinematic problem in the general case of separation of variables in the eikonal equation.

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Literature cited

  1. G. Herglotz, “Über das Benndorfsche Problem der Fortpflanzungsgeschwindigkeit der Erdbebenstrahlen,” Phys. Z.,8, No. 5, 145–147 (1907).

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  2. M. L. Gerver and V.M. Markushevich, “Hodograph determination of the propagation speed of seismic waves,” Vychisl. Seismologiya, Tr. Inst. Fiz. Zemli im. O. Yu. Shmidta Akad. Nauk. SSSR., No. 3, 3–51 (1967).

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  3. Yu. E. Anikonov, “Some particular solutions of the inverse kinematic problem,” Mat. Probl. Geofiz., Tr. VTs. Sib. Otd. Akad. Nauk SSSR, No. 4, 30–60 (1973).

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Additional information

Translated from Zapiski Nauchnykh Seminarov Leningradskogo Otdeleniya Matematichesko Instituta im. V. A. Steklova AN SSSR, Vol. 78, pp. 20–29, 1978.

The author thanks A. P. Kiselev for useful discussions during the course of the work and A. S. Blagoveshchenskii for valuable remarks made during reading the manuscript.

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Beil'kin, G.Y. Explicit solution of the inverse kinematic problem in the non-Herglotz case. J Math Sci 22, 1007–1014 (1983). https://doi.org/10.1007/BF01305283

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