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There are no conformal Einstein rescalings of complete pseudo-Riemannian Einstein metrics

机译:没有完整的伪黎曼爱因斯坦度量的保形爱因斯坦缩放

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Let g be an Einstein metric of indefinite signature such that the conformally-equivalent metric psi(-2) g is also Einstein. We show that if the metric g is light-line complete, then the conformal coefficient psi is constant. If the manifold is closed, the completeness assumption can be omitted (the latter result is due to Mikes-Radulovich and Kuhnel, but our proof is much simpler). The proof is based on the investigation of the behavior of the function psi along light-line geodesics: we show that for every light-line geodesic gamma(t) we have psi(gamma(t)) = const(1) . t + const(2). Since the function psi cannot vanish, the light-line completeness of the metric implies psi = const(2). If the manifold is closed, the function psi accepts its maximal value psi(max) at a certain point. Then, for every light-line geodesic gamma through this point we have const(1) = 0 implying psi = psi(max) at every point of this geodesic. Repeating the argumentation, we obtain that for every light-line geodesic gamma(1) intersecting gamma we have psi = psi(max) at every point of gamma(1) as well and so on. Since every two points can be connected by a sequence of light-line geodesics, psi is constant on the whole manifold. To cite this article: V. Kiosak, VS. Matveev, C R. Acad. Sci. Paris, Ser. 1347 (2009).
机译:令g为不确定签名的爱因斯坦度量,以使共形等效度量psi(-2)g也是爱因斯坦。我们表明,如果度量g是完整的直线,则保形系数psi是恒定的。如果歧管是封闭的,则可以省略完整性假设(后者的结果是由于Mikes-Radulovich和Kuhnel造成的,但是我们的证明要简单得多)。该证明基于对函数psi沿光线测地线的行为的调查:我们表明,对于每个光线测地线γ(t),我们都有psi(gamma(t))= const(1)。 t + const(2)。由于函数psi不会消失,因此度量标准的亮线完整性表示psi = const(2)。如果歧管关闭,则函数psi在特定点接受其最大值psi(max)。然后,对于通过该点的每个线状测地伽马,我们的const(1)= 0意味着在该测地线的每个点处psi = psi(max)。重复该论点,我们得出,对于相交于伽玛的每条光线线测地伽玛(1),在伽玛(1)的每个点处的psi = psi(max),依此类推。由于每两个点都可以通过一系列的灯光线测地线连接,因此psi在整个歧管上都是恒定的。引用本文:V. Kiosak,VS。 Matveev,C R. Acad。科学巴黎1347(2009)。

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