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A tensor over an <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/s/s085/s085730/s0857301.png" />-dimensional vector space <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/s/s085/s085730/s0857302.png" /> that is invariant under the operation of [[Alternation|alternation]] with respect to some group of its indices. The components of a skew-symmetric tensor are skew-symmetric with respect to the corresponding group of indices, i.e. if two indices are exchanged the components change sign (in the sense of the additive law of the field <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/s/s085/s085730/s0857303.png" /> over which <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/s/s085/s085730/s0857304.png" /> is defined), and if two indices are equal the components vanish.
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The most important skew-symmetric tensors are those that remain invariant under alternation with respect to the entire group of covariant or contravariant indices. A contravariant (covariant) skew-symmetric tensor of valency <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/s/s085/s085730/s0857305.png" /> is an <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/s/s085/s085730/s0857307.png" />-vector or multi-vector over <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/s/s085/s085730/s0857308.png" /> (respectively, over <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/s/s085/s085730/s0857309.png" />, the space dual to <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/s/s085/s085730/s08573010.png" />); they are elements of the exterior algebra of the vector space <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/s/s085/s085730/s08573011.png" />. The exterior algebra over <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/s/s085/s085730/s08573012.png" /> is usually called the algebra of exterior forms, identifying covariant skew-symmetric tensors of valency <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/s/s085/s085730/s08573013.png" /> with <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/s/s085/s085730/s08573014.png" />-forms.
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A tensor over an  $  n $-
 +
dimensional vector space  $  E $
 +
that is invariant under the operation of [[Alternation|alternation]] with respect to some group of its indices. The components of a skew-symmetric tensor are skew-symmetric with respect to the corresponding group of indices, i.e. if two indices are exchanged the components change sign (in the sense of the additive law of the field  $  K $
 +
over which  $  E $
 +
is defined), and if two indices are equal the components vanish.
 +
 
 +
The most important skew-symmetric tensors are those that remain invariant under alternation with respect to the entire group of covariant or contravariant indices. A contravariant (covariant) skew-symmetric tensor of valency $  r $
 +
is an $  r $-
 +
vector or multi-vector over $  E $(
 +
respectively, over $  E  ^ {*} $,  
 +
the space dual to $  E $);  
 +
they are elements of the exterior algebra of the vector space $  E $.  
 +
The exterior algebra over $  E  ^ {*} $
 +
is usually called the algebra of exterior forms, identifying covariant skew-symmetric tensors of valency $  r $
 +
with $  r $-
 +
forms.
  
 
For references see [[Exterior algebra|Exterior algebra]].
 
For references see [[Exterior algebra|Exterior algebra]].

Latest revision as of 08:14, 6 June 2020


A tensor over an $ n $- dimensional vector space $ E $ that is invariant under the operation of alternation with respect to some group of its indices. The components of a skew-symmetric tensor are skew-symmetric with respect to the corresponding group of indices, i.e. if two indices are exchanged the components change sign (in the sense of the additive law of the field $ K $ over which $ E $ is defined), and if two indices are equal the components vanish.

The most important skew-symmetric tensors are those that remain invariant under alternation with respect to the entire group of covariant or contravariant indices. A contravariant (covariant) skew-symmetric tensor of valency $ r $ is an $ r $- vector or multi-vector over $ E $( respectively, over $ E ^ {*} $, the space dual to $ E $); they are elements of the exterior algebra of the vector space $ E $. The exterior algebra over $ E ^ {*} $ is usually called the algebra of exterior forms, identifying covariant skew-symmetric tensors of valency $ r $ with $ r $- forms.

For references see Exterior algebra.

How to Cite This Entry:
Skew-symmetric tensor. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Skew-symmetric_tensor&oldid=48726
This article was adapted from an original article by I.Kh. Sabitov (originator), which appeared in Encyclopedia of Mathematics - ISBN 1402006098. See original article