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本文选择了一个特殊的、在任意座标变换下及局部Lorentz变换下不变的Lagrangian,着重讨论了在经典意义下的运动方程、给出了与Lagrangian相应的正则形式。In this paper, we suggest a Lagrangian which is invariant under the general coordinate transformation and local Lorentz transformation. The dicussion is focused on its classical Lagrangian equation of motion and the canonical formalism corresponding to this Lagraugian.
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