In mathematics, anticommutativity is a specific property of some non-commutative operations. In mathematical physics, where symmetry is of central importance, these operations are mostly called antisymmetric operations, and are extended in an associative setting to cover more than two arguments. Swapping the position of two arguments of an antisymmetric operation yields a result, which is the inverse of the result with unswapped arguments. The notion inverse refers to a group structure on the operation's codomain, possibly with another operation, such as addition.
Subtraction is an anticommutative operation because −(a − b) = b − a. For example, 2 − 10 = −(10 − 2) = −8.
A prominent example of an anticommutative operation is the Lie bracket.
More generally, a multilinear map is anticommutative if for all we have
where is the sign of the permutation .
If the abelian group has no 2-torsion, implying that if then , then any anticommutative bilinear map satisfies
More generally, by transposing two elements, any anticommutative multilinear map satisfies
if any of the are equal; such a map is said to be alternating. Conversely, using multilinearity, any alternating map is anticommutative. In the binary case this works as follows: if is alternating then by bilinearity we have
and the proof in the multilinear case is the same but in only two of the inputs.
Examples of anticommutative binary operations include:
- Exterior algebra
- Graded-commutative ring
- Operation (mathematics)
- Symmetry in mathematics
- Particle statistics (for anticommutativity in physics).
- Bourbaki, Nicolas (1989), "Chapter III. Tensor algebras, exterior algebras, symmetric algebras", Algebra. Chapters 1–3, Elements of Mathematics (2nd printing ed.), Berlin-Heidelberg-New York City: Springer-Verlag, ISBN 3-540-64243-9, MR 0979982, Zbl 0904.00001.
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