The Lorentzian scattering rigidity problem and rigidity of stationary metrics

Plamen Stefanov
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Abstract

We study scattering rigidity in Lorentzian geometry: recovery of a Lorentzian metric from the scattering relation \(\mathcal {S}^\sharp \) known on a lateral boundary. We show that, under a non-conjugacy assumption, every defining function r(xy) of the submanifold of pairs of boundary points which can be connected by a lightlike geodesic plays the role of the boundary distance function in the Riemannian case in the following sense. Its linearization is the light ray transform of tensor fields of order two which are the perturbations of the metric; and each one of \(\mathcal {S}^\sharp \) and r (up to an elliptic factor) determines the other uniquely. Next, we study scattering rigidity of stationary metrics in time-space cylinders and show that it can be reduced to boundary/lens rigidity of magnetic systems on the base; a problem studied previously. This implies several scattering rigidity results for stationary metrics.

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洛伦兹散射刚性问题与静止度量的刚性
我们研究洛伦兹几何中的散射刚性:从侧边界上已知的散射关系(\mathcal {S}^\sharp \)中恢复洛伦兹度量。我们证明,在非共轭假设下,边界点对的每一个定义函数r(x, y)都可以通过类似光的大地线连接起来,在以下意义上扮演黎曼情形中边界距离函数的角色。它的线性化是二阶张量场的光线变换,而二阶张量场是度量的扰动;并且 \(\mathcal {S}^\sharp \) 和 r(直到一个椭圆因子)中的每一个都唯一地决定另一个。接下来,我们研究时空圆柱体中静止度量的散射刚度,并证明它可以简化为底座上磁系的边界/透镜刚度;这是之前研究过的一个问题。这意味着静止度量的几个散射刚性结果。
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