首页> 外文期刊>Acta Applicandae Mathematicae: An International Journal on Applying Mathematics and Mathematical Applications >Lagrangian theory of tensor fields over spaces with contravariant and covariant affine connections and metrics and its application to Einstein's theory of gravitation in (V)over-bar(4) spaces
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Lagrangian theory of tensor fields over spaces with contravariant and covariant affine connections and metrics and its application to Einstein's theory of gravitation in (V)over-bar(4) spaces

机译:具有协变和协变仿射连接和度量的空间上的张量场的拉格朗日理论及其在(V)over-bar(4)空间中的爱因斯坦引力理论中的应用

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The Lagrangian formalism for tensor fields over differentiable manifolds with contravariant and covariant affine connections (whose components differ not only by sign) and a metric [((L)over-bar(n),g)-spaces] is considered. The functional, the Lie, the covariant, and the total variations of a Lagrangian density, depending on components of tensor fields (with finite rank) and their first and second covariant derivatives, are established. A variation operator is determined and the corollaries of its commutation relations with the covariant and the Lie differential operators are found. The canonical (common) method of Lagrangians with partial derivatives (MLPD) and the method of Lagrangians with covariant derivatives (MLCD) are outlined. They differ each other by the commutation relations the variation operator has to obey with the covariant and the Lie differential operator. The covariant Euler-Lagrange equations are found on the basis of the MLCD. The energy-momentum tensors are considered on the basis of the Lie variation and the covariant Noether identities. As an application of the investigated general scheme, (pseudo) Riemannian spaces with contravariant and covariant affine connections (whose components differ not only by sign) ((V)over-bar(n)-spaces) are considered as a special case of ((L)over-bar(n),g)-spaces with Riemannian metric, symmetric covariant connection and a weaker definition of dual vector basis with 'conformal' noncanonical contraction operator S(dx(i), partial derivative(j)) = dx(i)(partial derivative(j)) = e(phi(x)).g(j)(i). The geodesic and autoparallel equations in (V)over-bar(4)-spaces are found as different equations in contrast to the case of V-4 spaces. The Euler-Lagrange equations as Einstein's field equations in (V)over-bar(4)-spaces and the corresponding energy-momentum tensors (EMTs) are obtained and compared with the Einstein equations and the EMTs in V-4-spaces. The geodesic and the auto-parallel equations are discussed. [References: 34]
机译:考虑具有协变和协变仿射连接(其分量不仅因符号而异)和度量[[((L)over-bar(n),g)-spaces]的可分流形上张量场的拉格朗日形式主义。建立了张量密度的函数,Lie,协变和总变化,具体取决于张量场(具有有限秩)的分量及其一阶和二阶协变导数。确定变分算子,并找到其与协变和李微分算子的换向关系的推论。概述了带偏导数的Lagrangian的规范(通用)方法(MLPD)和带协变数的Lagrangian的方法(MLCD)。它们之间的差异在于,变差算子必须遵守协变和李微分算子的换向关系。在MLCD的基础上找到了协变Euler-Lagrange方程。能量动量张量是基于Lie变化和协变Noether身份来考虑的。作为研究的一般方案的一种应用,具有伪变和协变仿射连接(其分量不仅因符号而不同)的(伪)黎曼空间((V)over-bar(n)-空间)被视为( (L)具有黎曼度量,对称协变连接的超空间(n),g)空间,并且具有``保形''非规范收缩算子S(dx(i),偏导数(j))的对偶矢量基的定义较弱dx(i)(偏导数(j))= e(phi(x))。g(j)(i)。与V-4空间的情况相反,发现(V)over-bar(4)空间中的测地线方程和自平行方程为不同的方程。获得了在(V)over-bar(4)-空间中作为爱因斯坦场方程的Euler-Lagrange方程以及相应的能量动量张量(EMT),并将其与V-4空间中的爱因斯坦方程和EMT进行了比较。讨论了测地线方程和自动平行方程。 [参考:34]

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