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- Q6483803 subject Q6181442.
- Q6483803 subject Q8143802.
- Q6483803 subject Q8481600.
- Q6483803 subject Q8843496.
- Q6483803 subject Q8843500.
- Q6483803 abstract "The Lanczos tensor or Lanczos potential is a rank 3 tensor in general relativity that generates the Weyl tensor. It was first introduced by Cornelius Lanczos in 1949. The theoretical importance of the Lanczos tensor is that it serves as the gauge field for the gravitational field in the same way that, by analogy, the electromagnetic four-potential generates the electromagnetic field.".
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- Q6483803 wikiPageWikiLink Q558066.
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- Q6483803 wikiPageWikiLink Q6181442.
- Q6483803 wikiPageWikiLink Q686291.
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- Q6483803 wikiPageWikiLink Q742969.
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- Q6483803 wikiPageWikiLink Q7915800.
- Q6483803 wikiPageWikiLink Q8143802.
- Q6483803 wikiPageWikiLink Q832289.
- Q6483803 wikiPageWikiLink Q8481600.
- Q6483803 wikiPageWikiLink Q855112.
- Q6483803 wikiPageWikiLink Q869108.
- Q6483803 wikiPageWikiLink Q8843496.
- Q6483803 wikiPageWikiLink Q8843500.
- Q6483803 wikiPageWikiLink Q911268.
- Q6483803 comment "The Lanczos tensor or Lanczos potential is a rank 3 tensor in general relativity that generates the Weyl tensor. It was first introduced by Cornelius Lanczos in 1949. The theoretical importance of the Lanczos tensor is that it serves as the gauge field for the gravitational field in the same way that, by analogy, the electromagnetic four-potential generates the electromagnetic field.".
- Q6483803 label "Lanczos tensor".