Differential geometry MOC

Vielbein

A vielbein1 is a (local) orthonormal basis for a Semi-Riemannian manifold 𝑀. diff This amounts to being a local frame (π‘’πœ‡)π‘Ž satisfying

(π‘’πœ‡)π‘Ž(π‘’πœˆ)π‘Ž=πœ‚πœ‡πœˆ

for an appropriate diagonal β€œMinkowski” metric πœ‚.2 It immediately follows

(π‘’πœ‡)π‘Ž(π‘’πœˆ)𝑏=πœ‚πœ‡πœˆ(π‘’πœ‡)π‘Ž(π‘’πœˆ)𝑏=π›Ώπ‘Žπ‘.

Note that such a local frame is only unique up to a local Lorentz transformation or analogous group.

Index notation

This Zettel mixes Latin indices for abstract index notation and Greek indices for concrete indices with Einstein summation convention, sometimes within the same expression. Note that since the metric in this frame is πœ‚πœ‡πœˆ, this is the appropriate way to raise and lower concrete indices.

Curvature

Suppose βˆ‡ is the Levi-Civita connexion. The connexion 1-forms are defined by

πœ”πœ‡πœˆπ‘Ž=(π‘’πœ‡)π‘βˆ‡π‘Ž(π‘’πœˆ)π‘βˆˆΞ©1(𝑀).

We let πŽπœ‡πœˆ =πœ”πœ‡πœˆπ‘Ž and π’†πœ‡ =(π‘’πœ‡)π‘Ž. The compatibility with the metric becomes

πŽπœ‡πœˆ=βˆ’πŽπœˆπœ‡.

The torsion-free condition becomes

dπ’†πœ‡+πŽπœ‡πœˆβˆ§π’†πœˆ=0

^B1 becomes

π‘Ήπœ‡πœˆβˆ§π’†πœˆ=0

and ^B2 becomes

dπ‘Ήπœ‡πœˆ+πŽπœ‡πœŽβˆ§π‘ΉπœŽπœˆβˆ’π‘Ήπœ‡πœŽβˆ§πŽπœŽπœˆ.

Letting π‘Ήπœ‡πœˆ =π‘…πœ‡πœˆπ‘Žπ‘ ∈Ω2(𝑀) be the 2-form part of the Riemannian curvature, we have

π‘Ήπœ‡πœˆ=dπŽπœ‡πœˆ+πŽπœ‡πœŽβˆ§πŽπœŽπœˆ.


develop | en | SemBr

Footnotes

  1. Physicists often call this a non-coΓΆrdinate basis, even though not being a coΓΆrdinate basis is insufficient to guarantee this property. ↩

  2. If 𝑀 is a Riemannian manifold we take the Kronecker delta. Otherwise πœ‚ is chosen so that its signature matches 𝑔. ↩