Work with modulo and modulo . By Fermat's little theorem, in , so the factor is independent of the chosen representative of . The proposed multiplication is therefore well defined on the stated Cartesian product. Its two associative bracketings have the same second component:
and both have first component . The identity element is , and the two-sided inverse element is
Thus the multiplication defines the twisted cyclic pair group, of order .
If , multiplication is coordinatewise addition, so the group is abelian. If , then and both and are available; their products in opposite orders are and . They differ. Hence
Both and contain the identity element and are closed under the multiplication and inverses: they are the cyclic groups of orders and respectively. Conjugation gives, with all coordinates reduced in the appropriate modulus,
so is a normal subgroup. For , the corresponding calculation is
When this lies in . Conversely, for , take , , : the second coordinate is , so is not normal. Thus is normal precisely when .
Finally, the projection
is a surjective group homomorphism because the first coordinates add. Its kernel of a group homomorphism is exactly . At , is the only possibility and the first factor is trivial, consistent with every conclusion. No assumption that generates the multiplicative group of the finite field is needed.
A real Lie group is a finite-dimensional real smooth manifold with a group structure whose multiplication and inversion are smooth. Its tangent space at the identity element is the vector space of velocities of smooth curves through . For the general linear group it identifies with . The matrix exponential and local matrix logarithm are
The exponential is globally defined, and each matrix is invertible with inverse . The logarithm here is a local map near ; it is not a globally defined inverse on every real invertible matrix. The differential of at zero is the identity, and the two power series are inverse locally.
For a general , the assumed Exponential map of a Lie group with has a smooth local inverse by the inverse function theorem, giving a local exponential chart. Define the Lie bracket from local group commutators by
For small the group commutator lies in that chart. More explicitly, the map is smooth and has . Its mixed second differential at is a bilinear map of , proving bilinearity. Swapping the two group elements inverts the commutator, and near . Thus and . In the matrix group, expansion to the mixed term gives the familiar commutator .
For , let and define the Adjoint representation of a Lie group by . It is smooth and satisfies . Its derived representation is . Naturality of the Exponential map of a Lie group under conjugation gives
At , the derivative of the logarithm of the commutator is : the derivative of multiplication at adds tangent vectors, and . Differentiate in to conclude
To prove the Jacobi identity without assuming it in the bracket construction, first establish that the differential of a Lie group homomorphism preserves Lie brackets. For a homomorphism , the allowed exponential identity gives locally. Apply this identity to the group commutator and take the mixed derivative to obtain . In particular gives
Applying both sides to yields . Rearranging with antisymmetry proves
Neither injectivity of nor the existence of a global logarithm was used.
Finally let be a normal Lie subgroup of , with its corresponding Lie algebra . For each , conjugation restricts to , so its differential preserves : . Differentiate along to get for every and . Thus the Lie algebra of a normal Lie subgroup is an ideal of a Lie algebra. The assertion concerns a subgroup carrying the corresponding Lie-subgroup structure, for example any closed subgroup; no arbitrary abstract subgroup is being assigned a tangent space.
Suppose every group commutator belongs to . For and , the particular group commutator belongs to . Multiplying on the left by gives . Thus for every ; applying the same inclusion to gives the reverse inclusion. Therefore is a normal subgroup.
We can now form the quotient group. Its group commutators are
A group commutator is the identity element exactly when the two elements commute. Hence is an abelian group. Equivalently, the hypothesis says that contains the commutator subgroup, so the quotient factors through the abelianization.
Use the class equation for the action of on itself by conjugation:
where the sum runs over noncentral conjugacy classes. By Lagrange's theorem, each noncentral class has size a positive power of greater than one. Thus . Since the identity element belongs to the center of a group,
For , the possible orders of the center of a group are . Order would make an abelian group. Order would make the quotient group have prime order and hence be a cyclic group. But a cyclic quotient by the center forces to be Abelian: if generates the quotient, any two elements are and with , and their products commute. Both larger orders contradict the hypothesis. Consequently
The Noncommutative Ruzsa triangle inequality says that nonempty finite subsets of a group satisfy
The Ruzsa covering lemma says that if , then some with satisfies
Now let be a symmetric subset of a group, so and . Apply the triangle inequality with the middle set to obtain, for ,
The hypothesis therefore gives . Starting from proves
In particular . Apply the covering lemma to and . There is with such that
The set is symmetric and contains the identity element, so this inclusion is exactly the covering condition showing that
Small doubling alone is insufficient in a noncommutative group. Let be a finite group, let be its free product with an infinite cyclic group, and put
Then is symmetric and , while contains the double coset . Distinct pairs give distinct reduced words , so . Letting proves the small doubling does not control tripling in a noncommutative group phenomenon.
The order of a group element is the least positive integer such that , where is the identity element; its order is infinite if no such exists.
Let have finite order . A group homomorphism preserves the group operation and the identity, so
The order of an element divides every positive exponent that gives the identity. Hence
If is a surjective function and has order , choose with . The first result gives , where . The element
then has order , because the order of is .
A group homomorphism is determined by the image of a generator of the cyclic group , and that image must have order dividing . In the symmetric group , the only such elements are the identity and the three-cycles. There are
three-cycles. Therefore the number of homomorphisms is
A subset of a multiplicatively written group is symmetric when it contains the identity element and . Consequently .
Torsion-free group 2026-10-03
A torsion-free group is a group in which the identity element is the only element of finite order of a group element.