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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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rdfs:label	Lanczos tensor (en)
rdfs: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. (en)
dcterms:subject	1949 introductions Differential geometry Gauge theories Tensors in general relativity Tensors
Wikipage page ID	2403085 (xsd:integer)
Wikipage revision ID	1108571887 (xsd:integer)
Link from a Wikipage to another Wikipage	Schwarzschild metric Electromagnetic field Electromagnetic four-potential Antisymmetric tensor Homogeneous differential equation Ricci calculus Curtright field D'Alembert operator Vector field Electromagnetic wave 1949 introductions Differential geometry Gauge theories Cornelius Lanczos Einstein field equations General relativity Gravitational field Gravitational wave Affine group Tensors in general relativity Bach tensor Cotton tensor Covariant derivative Tensor rank Tensors Lagrange multiplier Symmetric tensor Spacetime Natural units Self-dual Palatini action Schouten tensor Petrov type D Newman–Penrose formalism Weyl tensor Vacuum solution (general relativity) Ricci decomposition Tetradic Palatini action Variational methods in general relativity Riemann tensor Gauge field Gauge freedom Ricci tensor
Link from a Wikipage to an external page	http://www.worldscibooks.com/physics/5222.html
sameAs	Lanczos tensor Lanczos tensor Lanczos tensor Lanczos tensor
dbp:wikiPageUsesTemplate	dbt:Reflist dbt:Short_description
has 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. (en)
gold:hypernym	Tensor
prov:wasDerivedFrom	wikipedia-en:Lanczos_tensor?oldid=1108571887&ns=0
page length (characters) of wiki page	11663 (xsd:nonNegativeInteger)
foaf:isPrimaryTopicOf	wikipedia-en:Lanczos_tensor
is Link from a Wikipage to another Wikipage of	List of contributors to general relativity 1949 in science Curtright field Index of physics articles (L) Timeline of gravitational physics and relativity Cornelius Lanczos Gauge theory Dual graviton Linearized gravity Weyl tensor Tetradic Palatini action Lanczos potential Lanczos potential tensor Lanczos spintensor Weyl-Lanczos equation Weyl-Lanczos equations Weyl–Lanczos equation Weyl–Lanczos equations
is Wikipage redirect of	Lanczos potential Lanczos potential tensor

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