Anticommutative property

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In mathematics, anticommutativity is a specific property of some non-commutative mathematical operations. 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. Subtraction is an anticommutative operation because commuting the operands of ab gives ba=(ab); for example, 210=(102)=8. Another prominent example of an anticommutative operation is the Lie bracket.

In mathematical physics, where symmetry is of central importance, or even just in multilinear algebra these operations are mostly (multilinear with respect to some vector structures and then) called antisymmetric operations, and when they are not already of arity greater than two, extended in an associative setting to cover more than two arguments.

Definition

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If A,B are two abelian groups, a bilinear map f:A2B is anticommutative if for all x,yA we have

f(x,y)=f(y,x).

More generally, a multilinear map g:AnB is anticommutative if for all x1,xnA we have

g(x1,x2,xn)=sgn(σ)g(xσ(1),xσ(2),xσ(n))

where sgn(σ) is the sign of the permutation σ.

Properties

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If the abelian group B has no 2-torsion, implying that if x=x then x=0, then any anticommutative bilinear map f:A2B satisfies

f(x,x)=0.

More generally, by transposing two elements, any anticommutative multilinear map g:AnB satisfies

g(x1,x2,xn)=0

if any of the xi 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 f:A2B is alternating then by bilinearity we have

f(x+y,x+y)=f(x,x)+f(x,y)+f(y,x)+f(y,y)=f(x,y)+f(y,x)=0

and the proof in the multilinear case is the same but in only two of the inputs.

Examples

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Examples of anticommutative binary operations include:

See also

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References

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