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首页> 外文期刊>Journal of Mathematical Physics >Covariant differential identities and conservation laws in metric-torsion theories of gravitation. II. Manifestly generally covariant theories
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Covariant differential identities and conservation laws in metric-torsion theories of gravitation. II. Manifestly generally covariant theories

机译:引力度量扭理论中的协变微分恒等式和守恒律。二。显然是协变理论

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The present paper continues the work of Lompay and Petrov [J. Math. Phys.54, 062504 (2013)] where manifestly covariant differential identities and conserved quantities in generally covariant metric-torsion theories of gravity of the most general type have been constructed. Here, we study these theories presented more concretely, setting that their Lagrangians L are manifestly generally covariant scalars: algebraic functions of contractions of tensor functions and their covariant derivatives. It is assumed that Lagrangians depend on metric tensor g, curvature tensor R, torsion tensor T and its first ?T and second ??T covariant derivatives, besides, on an arbitrary set of other tensor (matter) fields φ and their first ?φ and second ??φ covariant derivatives: L=L(g,R;T,?T,??T;φ,?φ,??φ). Thus, both the standard minimal coupling with the Riemann-Cartan geometry and non-minimal coupling with the curvature and torsion tensors are considered. The studies and results are as follow: (a) A physical interpretation of the Noether and Klein identities is examined. It was found that they are the basis for constructing equations of balance of energy-momentum tensors of various types (canonical, metrical, and Belinfante symmetrized). The equations of balance are presented. (b) Using the generalized equations of balance, new (generalized) manifestly generally covariant expressions for canonical energy-momentum and spin tensors of the matter fields are constructed. In the cases, when the matter Lagrangian contains both the higher derivatives and non-minimal coupling with curvature and torsion, such generalizations are non-trivial. (c) The Belinfante procedure is generalized for an arbitrary Riemann-Cartan space. (d) A more convenient in applications generalized expression for the canonical superpotential is obtained. (e) A total system of equations for the gravitational fields and matter sources are presented in the form more naturally generalizing the Einstein-Cartan equations with matter. This result, being a one of the more important results itself, is to be also a basis for constructing physically sensible conservation laws and their applications.
机译:本论文继续了Lompay和Petrov的工作[J.数学。 Phys.54,062504(2013)],其中在最一般类型的重力的一般协变度量-扭转理论中,构造了明显的协变微分恒等式和守恒量。在这里,我们将更具体地研究这些理论,并确定它们的拉格朗日L显然是一般的协变标量:张量函数压缩的代数函数及其协变导数。假定拉格朗日依赖于度量张量g,曲率张量R,扭转张量T及其一阶?T和二阶?? T协变量导数,此外还取决于任意一组其他张量(物)场φ及其第一φ第二个Δφφ协变导数:L = L(g,R; T,ΔT,ΔT;φ,Δφ,Δφφ)。因此,考虑了与黎曼-卡坦几何学的标准最小耦合和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)使用一般的平衡方程,构造出新的(一般化的)明显的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曲率和扭转的非最小耦合时,这种概括是不平凡的。 (c)将Belinfante程序推广到任意Riemann-Cartan空间。 (d)在应用中获得了更方便的规范超势的广义表达。 (e)引力场和物质源的总方程组以更自然的形式概括了物质的爱因斯坦-卡坦方程。这一结果本身就是更重要的结果之一,也将成为构建物理上合理的保护法则及其应用的基础。

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