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Covariant Differential Identities and Conservation Laws in Metric-Torsion Theories of Gravitation. II. Manifestly Generally Covariant Theories

机译:协变差分恒等式和守恒定律   引力的公制 - 扭转理论。 II。显然通常是协变的   理论

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摘要

The present paper continues the work of the authors [arXiv:1306.6887[gr-qc]]. Here, we study generally covariant metric-torsion theories of gravitypresented more concretely, setting that their Lagrangians are \emph{manifestly}generally covariant scalars. It is assumed that Lagrangians depend on metrictensor, curvature tensor, torsion tensor and its first and second covariantderivatives, besides, on an arbitrary set of other tensor (matter) fields andtheir first and second covariant derivatives. Thus, both the standard minimalcoupling with the Riemann-Cartan geometry and non-minimal coupling with thecurvature and torsion tensors are considered. The studies and results are as follow. (a) A physical interpretation of theNoether and Klein identities is examined. It was found that they are the basisfor constructing equations of balance of energy-momentum tensors of varioustypes (canonical, metrical and Belinfante symmetrized). The equations ofbalance are presented. (b) Using the generalized equations of balance, new(generalized) manifestly generally covariant expressions for canonicalenergy-momentum and spin tensors of the matter fields are constructed. In thecases, when the matter Lagrangian contains both the higher derivatives andnon-minimal coupling with curvature and torsion, such generalizations arenon-trivial. (c) The Belinfante procedure is generalized for an arbitraryRiemann-Cartan space. (d) A more convenient in applications generalizedexpression for the canonical superpotential is obtained. (e) A total system ofequations for the gravitational fields and matter sources are presented in theform more naturally generalizing the Einstein-Cartan equations with matter.This result, being a one of more important results itself, is to be also abasis for constructing physically sensible conservation laws and theirapplications.
机译:本文继续了作者的工作[arXiv:1306.6887 [gr-qc]]。在这里,我们研究一般更具体表示的重力协变度量扭转理论,设置它们的拉格朗日数为\ emph {明显地}一般为协变标量。假定拉格朗日依赖于度量张量,曲率张量,扭转张量及其第一和第二协变导数,此外还依赖于任意其他张量(物)场及其第一和第二协变导数。因此,考虑了与黎曼-卡坦几何学的标准最小耦合以及与曲率和扭转张量的非最小耦合。研究和结果如下。 (a)检查了Noether和Klein身份的物理解释。发现它们是构造各种类型的能量动量张量平衡方程的基础(规范的,度量的和贝林芬特对称的)。提出了平衡方程。 (b)使用广义的平衡方程,构造出新的(广义的)明显地规范能量动量和物质场自旋张量的协变表达式。在这种情况下,当拉格朗日物质既包含高阶导数又包含具有曲率和扭转的非最小耦合时,这种推广是不平凡的。 (c)Belinfante程序适用于任意黎曼-卡坦空间。 (d)在应用中获得了规范正则势的广义表达式更方便的方法。 (e)引力场和物质源的总方程组以更自然地概括了物质的爱因斯坦-卡坦方程的形式给出,这一结果本身就是更重要的结果之一,也是构造物理上有意义的基础守恒定律及其应用

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