For indices in , this Levi-Civita symbol is zero when any indices repeat, and otherwise is the sign of a permutation taking to . Thus and exchanging any two index slots changes the sign. It expresses a determinant as with repeated indices summed. Exactly components are nonzero, so .
The determinant transformation formula for the Levi-Civita symbol shows that it is invariant under every proper rotation matrix, for which . Under an orthogonal reflection its sign reverses. This distinguishes proper-rotation isotropy from the pseudotensor transformation convention when both orientations are included.
Contracting one index gives
For a matrix , contraction of with proves the title identity, because . DefineExpansion shows that is the cofactor matrix. Equivalently, the determinant identity gives . Thus for invertible ,Differentiating the cubic determinant formula gives three equal terms, so . This is the entrywise derivative of the determinant and remains valid for singular through the cofactor expression. The inverse expression requires .
For real three-dimensional vectors, Lagrange's identity gives with symmetric matrix . For , the normal line spanned by is its kernel and the perpendicular plane is its eigenspace. Consequently is positive semidefinite, has rank two and has zero determinant. For , it is the zero matrix.
For three vectors in oriented Euclidean three-space, the scalar triple product is and the vector triple product is . The former is their signed volume; the latter is the vector operation appearing in the vector triple product identity.
Contracting two Levi-Civita symbols gives
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The Levi-Civita symbol, denoted as \(\epsilon_{ijk}\) in three dimensions or \(\epsilon_{i_1 i_2 \ldots i_n}\) in \(n\) dimensions, is a mathematical object used in tensor analysis and differential geometry.
Definition:
- odd permutation: -1
- even permutation: 1
- not a permutation: 0. This happens iff two more more indices are repeated