Thomas-Whitehead重力的一般结构

Samuel Brensinger, K. Heitritter, V. Rodgers, K. Stiffler
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引用次数: 2

摘要

Thomas-Whitehead (TW)引力是d维流形上的引力投影不变模型,它通过重参数化不变性与弦理论密切相关。非参数化测地线是将弦理论和高维引力联系在一起的无处不在的结构。这是通过特雷西·托马斯的投影几何来实现的。由Thomas和后来的Whitehead提出的射影联系,承认了一个在一维中与Virasoro代数的辅元一对一对应的分量。这个分量在文献中称为微分同态域$\mathcal{D}_{ab}$。在四维空间中,当$\math {D}_{ab}$与爱因斯坦度规成正比时,TW\作用坍缩为具有宇宙常数的爱因斯坦-希尔伯特作用。这些先前的结果要么局限于特定的度量,如Polyakov二维度量,要么局限于保持体积的坐标。本文综述了TW重力,并推导了TW作用的规范不变量,它是显射影不变量和一般坐标不变量。我们推导了TW作用的协变场方程,并展示了费米子场如何与规范不变理论耦合。独立域是度量张量$g_{ab}$,基本射影不变量$\Pi^{a}_{\,\,\,bc}$和微分同构域$\数学D_{ab}$。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
General structure of Thomas-Whitehead gravity
Thomas-Whitehead (TW) gravity is a projectively invariant model of gravity over a d-dimensional manifold that is intimately related to string theory through reparameterization invariance. Unparameterized geodesics are the ubiquitous structure that ties together string theory and higher dimensional gravitation. This is realized through the projective geometry of Tracy Thomas. The projective connection, due to Thomas and later Whitehead, admits a component that in one dimension is in one-to-one correspondence with the coadjoint elements of the Virasoro algebra. This component is called the diffeomorphism field $\mathcal{D}_{ab }$ in the literature. It also has been shown that in four dimensions, the TW\ action collapses to the Einstein-Hilbert action with cosmological constant when $\mathcal{D}_{ab}$ is proportional to the Einstein metric. These previous results have been restricted to either particular metrics, such as the Polyakov 2D\ metric, or were restricted to coordinates that were volume preserving. In this paper, we review TW gravity and derive the gauge invariant TW action that is explicitly projectively invariant and general coordinate invariant. We derive the covariant field equations for the TW action and show how fermionic fields couple to the gauge invariant theory. The independent fields are the metric tensor $g_{ab}$, the fundamental projective invariant $\Pi^{a}_{\,\,\,bc}$, and the diffeomorphism field $\mathcal D_{ab}$.
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