Abstract
By the classical differential geometry techniques it is shown that a general partial differential equation of the second order with two independent variables can be represented in the Lax operator form [X 1 X 2]=0, whereX i =∂/∂x i −Ω i,i=1,2 andΩ i are the 3×3 matrices. The problem of the introduction of the spectral parameter in this representation is shortly discussed.
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References
Ablowitz M. J., Kaup D. J., Newell A. C., Segur H.: Stud. Appl. Math.53 (1974) 249.
Mel'nikov V. K.: Physics of elementary particles and atomic nuclei11 (1980) 1224 (in Russian).
Scott A. C., Chu F. Y. F., McLaughlin D. W.: Proc. IEEE61 (1973) 1443.
Wahlquist H. D., Estabrook F. B.: J. Math. Phys.16 (1975) 1.
Lund F.: Phys. Rev. D15 (1977) 1540.
Sasaki R.: Nucl. Phys. B154 (1979) 343.
Barbashov B. M., Nesterenko V. V.: Fortschritte der Physik28 (1980) 427.
Eisenhart L. P.: An Introduction to Differential Geometry with Use of the Tensor Calculus, Princeton University Press, Princeton, 1940.
Pohlmeyer K.: Commun. Math. Phys.46 (1976) 209.
Neveu A., Papanicolaou N.: Commun. Math. Phys.58 (1976) 31.
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The author is pleased to thank V. K. Mel'nikov for the discussion of this work.
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Nesterenko, V.V. On the Lax representation for the nonlinear evolution equations. Czech J Phys 32, 668–671 (1982). https://doi.org/10.1007/BF01596714
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DOI: https://doi.org/10.1007/BF01596714