Toy Universes

Gravity inside our minds

Notation

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[This page is under construction].

  • We use Einstein’s summation convention.
  • We adopt the metric signature (-,+,+,+).
  • We generally adopt the notation of [MTW73], unless explicitly stated otherwise.
  • Tensors will be treated either by “index free” (geometrical) notation or “classical component” (index) notation, or both, depending on the point that is being addressed/emphasized. Tags denoted “Index-Free” and “Full-Index” will be used to indicate appropriately.
  • In our initial discussions on tensors, you will also see that we will be using an unorthodox notation for tensors, particularly for Euclidean tensors. Given an Euclidean tensorTof rankp=n+m, it hasninput slots (operates onnvectors\vec{v}_1, \dots, \vec{v}_n) and outputs another tensor of rankm. We write the tensorTas: T_{\xrightarrow{n,m}} (\vec{v}_1, \dots, \vec{v}_n) . That notation will be dropped later.
  • We adopt any of the following notations for the Cartesian (orthonormal) basis vectors and for the components of a vector\vec{u}in that basis, respectively:\hat{e}_x \equiv \hat{e}_i  \equiv \hat{\rm i},
    \hat{e}_y \equiv \hat{e}_j \equiv \hat{\rm j},
    \hat{e}_z \equiv \hat{e}_k \equiv \hat{\rm k},

    u_x \equiv (\vec{u})_x \equiv (\vec{u})_i \equiv u_i,
    u_y \equiv (\vec{u})_y \equiv (\vec{u})_j \equiv u_j,
    u_z \equiv (\vec{u})_z \equiv (\vec{u})_k \equiv u_k.

  • A tensor \mathbf{T} of type \binom{N}{N^{\prime}} at a point P of  a manifold is a linear function that takes as its arguments N one-forms and N^{\prime} vectors. We also write it as \mathbf{T}(\tilde{\omega}_{(1)}, \dots,  \tilde{\omega}_{(N)}; v_{(1)}, \dots, v_{(N^{\prime})}).

Written by Christine

December 19, 2010 at 6:36 PM

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