A Lie algebra is a vector space (over a field; we'll usually use π or π ) π€ equipped with an operation [-,-]:π€Γπ€βπ€ satisfying:
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bilinearity (over our chosen field k ), that is the ability to expand brackets: [aX+bY,Z]=a[X,Z]+b[Y,Z] and [X,aY+bZ]=a[X,Y]+b[X,Z]βX,Y,Zβπ€,a,bβk
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for all Xβπ€ we require [X,X]=0 . This makes sense if you think about the commutator bracket, because [X,X]=XX-XX=0 .
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the Jacobi identity: [X,[Y,Z]]+[Y,[Z,X]]+[Z,[X,Y]]=0βX,Y,Zβπ€.
To remember this formula, note that the second and third terms are cyclic permutations of the first.