General Relativity and John Archibald Wheeler by Ignazio Ciufolini & Richard A. Matzner
Author:Ignazio Ciufolini & Richard A. Matzner
Language: eng
Format: epub
Publisher: Springer Netherlands, Dordrecht
Of course, the ζ-Laplaceequation reduces for ζ2 = − 1 to the ordinary Laplace equation, while for ζ2 = 1 to the wave equation. The operator − ζ2 ∂ x 2 + ∂ y 2 will be called the ζ-Laplace operator.
In the following a ζ-complex structure on will denote an endomorphism of the module of all vector fields on , with J 2 = ζ2 I, J≠0, I, and vanishing Nijenhuis torsion, i.e., J, J FN = 0, where ⋅, ⋅ FN denotes for the Frölicher–Nijenhuis bracket. A 2-dimensional manifold supplied with a ζ-complex structure is called a ζ-complex curve.
Obviously, for ζ2 = − 1 a ζ-complex curve is just an ordinary 1 − dimensional complex manifold (curve).
By using the endomorphism J the ζ-Laplace equation can be written intrinsicallyas
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