Massless Lorentz gauge field consistent with Einstein's gravitation theory. The case \(\alpha+2a/3=\beta-2a/3=\gamma+3a/2=0\) (Q2769953)
From MaRDI portal
 | This is the item page for this Wikibase entity, intended for internal use and editing purposes. Please use this page instead for the normal view: Massless Lorentz gauge field consistent with Einstein's gravitation theory. The case \(\alpha+2a/3=\beta-2a/3=\gamma+3a/2=0\) |
scientific article; zbMATH DE number 1702400
| Language | Label | Description | Also known as |
|---|---|---|---|
| English | Massless Lorentz gauge field consistent with Einstein's gravitation theory. The case \(\alpha+2a/3=\beta-2a/3=\gamma+3a/2=0\) |
scientific article; zbMATH DE number 1702400 |
Statements
6 February 2002
0 references
Massless Lorentz gauge field consistent with Einstein's gravitation theory. The case \(\alpha+2a/3=\beta-2a/3=\gamma+3a/2=0\) (English)
0 references
