By Lagrange's theorem, a stabilizer subgroup of has order for some . The orbit-stabilizer theorem therefore gives
Thus an orbit of a group action either has one element or has size divisible by , even if the acted-on set is infinite.
Apply this to the conjugation action. Its singleton orbits of a group action are the elements of the centre of a group, while every other orbit has size divisible by . Partitioning the finite group into these orbits gives the class equation, and hence
Since the identity belongs to , its order is positive and divisible by . Consequently
Now suppose that . It is then proper, so choose . The centralizer
is a subgroup: commuting with is preserved by multiplication and inverses. It contains and also , so . By Lagrange's theorem, its order is a power of dividing , forcing . But that would make central, a contradiction. Therefore
A simple group has no normal subgroup except the identity subgroup and the whole group. To prove the Simplicity of the alternating group A5, we compute its conjugacy classes. Since the sign homomorphism is onto, . Its possible nonidentity cycle types are a three-cycle, a product of two disjoint transpositions, and a five-cycle.
There are three-cycles. The centralizer in of consists of its three powers and an independent interchange of the two unused letters. Only the three powers are even. Its centralizer in therefore has order three, giving one conjugacy class of size by the orbit-stabilizer theorem.
There are products of two disjoint transpositions: choose the fixed letter and then a pairing of the other four letters. For , a commuting permutation fixes and may interchange the two pairs and swap within them, giving a centralizer of order eight in . It contains an odd element, , so exactly half its elements are even. The centralizer in has order four, and these fifteen elements form one conjugacy class of size .
Finally, there are five-cycles. A permutation commuting with a five-cycle is determined by the image of one letter and must be a power of that cycle. All five powers are even, so the centralizer in has order five. Each such conjugacy class has size , giving two classes of size twelve.
A normal subgroup must be a union of conjugacy classes and must include the identity. Its order therefore has the form
The resulting distinct possibilities are
Of these, only and divide . Lagrange's theorem rules out every other possible order. Hence
A permutation cycle sends to , each successive listed point to the next, and to , fixing every unlisted point. Its length is . For any permutation ,
Thus conjugate group elements in the symmetric group have the same cycle length. Conversely, two cycles of the same length are conjugate: send their entries, in cyclic order, to one another and extend this bijection arbitrarily to the unused points. Length-one cycles represent the identity and cause no exception to this conclusion.
An odd-length permutation cycle is an even permutation, since its sign is . Let be such cycles on points and choose with . If is odd, let be the transposition of the two points unused by the listed cycle . Then , and is even with
Hence all the -cycles are conjugate within . The two spare letters supply the parity correction; they are the reason the same argument need not work with only one spare letter.
In the answer is no. For example, and are conjugated by the odd transposition in . The centralizer of in is exactly its order-three cyclic subgroup: a commuting permutation fixes the unique fixed point and acts as a power of the cycle on the other three points. All these centralizing elements are even. Every other conjugating element differs from by a centralizing element, so it is also odd. There is no conjugator in . Equivalently, the eight three-cycles split into two conjugacy classes of size , illustrating the alternating conjugacy class splitting criterion.
The conjugacy class of is its orbit under the conjugation action, and its stabilizer is the centralizer . The orbit-stabilizer theorem gives
By Lagrange's theorem, the order of the centralizer divides , so the index is a power of . A conjugacy class has size one exactly when its element belongs to the center of a group.
Separate these singleton classes in the class equation:
where the sum takes one representative of each nonsingleton conjugacy class. Every summand is divisible by . Thus , and the identity ensures . Consequently . This is the nontrivial center of a finite p-group property.
A soluble group, also called a solvable group, has a terminating derived series:
For a subgroup , induction gives , so subgroups of soluble groups are soluble. For a surjective group homomorphism , , so quotients of soluble groups are soluble. Finally, in a group extension , suppose and . Then and . Soluble groups are closed under subgroups, quotients and group extensions.
A virtually soluble group contains a soluble group as a finite-index subgroup. The finite-index facts proved in parts (i)–(iii) imply closure under subgroups and quotients: intersect a finite-index soluble subgroup with the chosen subgroup, or take its image under the quotient map.
For group extensions, no finite-generation hypothesis may be inserted. We first establish the finite-index characteristic soluble subgroup lemma. If is a virtually soluble group, the kernel of its action on the cosets of a finite-index soluble subgroup is a soluble normal subgroup of finite index. Among soluble normal subgroups containing , choose with maximal , possible because is finite. If is any soluble normal subgroup of , then is soluble: it is an extension of by . Maximality forces . Thus is the unique largest soluble normal subgroup of , making it a characteristic subgroup, and it has finite index.
Now suppose has both and virtually soluble. Replace by the preimage of a finite-index soluble subgroup of . The subgroup just constructed is characteristic in and therefore normal in . In , the subgroup is a finite normal subgroup, and is a soluble group. The centralizer has finite index in , since conjugation gives a map with finite image. Its intersection with is the center of a group , an abelian group, while its quotient by embeds in the soluble group . Thus is a soluble group. Its preimage in is an extension by , so it too is soluble and has finite index in . Virtually soluble groups are closed under group extensions.
For the final example take the restricted direct sum of groups
where is the nonabelian simple group of even permutations on five letters. Every finite collection of elements lies in a product of finitely many finite factors, so is a locally finite group and hence a torsion group. It cannot contain a nonabelian free group, which is a torsion-free group.
To show that is not a virtually soluble group, let be any finite-index subgroup and let be the kernel of the finite coset action. Each coordinate maps either injectively or trivially into the finite quotient , by Simplicity of the alternating group A5. The nontrivial images of distinct factors commute, and each has trivial centre, so any of them generate a direct product of groups of order . Only finitely many such images can occur in a finite quotient. Therefore , and hence , contains a whole coordinate copy of , which is not soluble: its nontrivial commutator subgroup is normal and therefore equals . No finite-index subgroup of is soluble.
The identity belongs to the center of a group. If commute with every , then does too; rearranging also shows that commutes with . Hence is a subgroup. Moreover for , so it is a normal subgroup.
Suppose . The conjugation action partitions into conjugacy classes. The orbit-stabilizer theorem gives class size , where is the centralizer of . By Lagrange's theorem, this size is a power of ; it is one exactly when is central. Thus the class equation has the form
It follows that . Since the identity is central, , and therefore
This is the nontrivial-centre property of a finite p-group.
The printed uniqueness assertion has an exceptional case at . To locate it, use the two double cosets
An -bimodule-equivariant set map is determined by and . Equivariance requires and
because and commutes with this subgroup. These conditions are also sufficient: define and . Changing the double-coset expression only inserts an element of , which commutes with .
For , the center of and this centralizer are both trivial. For the latter, a commuting permutation must fix the unique point outside and lie in the center of ; that center is trivial when . Therefore , giving deletion. For , however, . The choice
is well defined and satisfies all the printed equivariance conditions, but sends to rather than to the identity. Uniqueness holds for ; it is false at as printed. Even requiring the map to restrict to the identity on does not remove this counterexample.
In the matrix expression, denotes a fundamental generator, whereas the component adjoint covariant derivative uses adjoint generators. With ,
Using antisymmetry to write and gives exactly the component mass term. This is the gauge-boson mass matrix from an adjoint scalar.
For , the Gell-Mann matrices commute with . Their gauge bosons are therefore massless. The generators connect the first two eigenspaces to the third; the eigenvalue difference is . Directly taking the matrix trace gives
with all remaining entries zero. Thus
The factor is the canonical real-vector mass term normalization. The unbroken Lie algebra is , giving the usual description SU(2) × U(1). More precisely, the centralizer of the vacuum expectation value inside is
This global quotient refines the adjoint-Higgs breaking of SU(3) to SU(2) and U(1) without changing the local gauge boson spectrum.
Conjugating a cycle merely relabels its entries:
Thus conjugate permutations have the same cycle type. Conversely, if and have the same cycle type, match the entries of each cycle of bijectively and in cyclic order with those of a cycle of of the same length. Extending these matches to a permutation gives .
Let be the centralizer of . Its -conjugacy class remains one -conjugacy class exactly when contains an odd permutation. Indeed, in that case has index two in , so the orbit-stabilizer theorem gives
If the centralizer contains only even permutations, the class has half the size and the class splits into two classes.
The even cycle types in are
The classes of the identity, a three-cycle, and a double transposition do not split: their centralizers contain an odd permutation. The centralizer of a five-cycle is its cyclic subgroup of order five, which lies in , so that class splits in two. Therefore
For , the root-space decomposition gives its centralizer
Every root space is one-dimensional, so this centralizer has the minimum possible dimension exactly when no summand on the right occurs. By the Regular element criterion in a Cartan subalgebra,
Let act on the group algebra by conjugation. Its fixed-point algebra is
and the centralizer consists of the elements of commuting with every element of . The Brauer morphism is
Thus deletes the coefficients of basis elements outside . The nonfixed -orbits have cardinality divisible by , so the usual orbit argument shows that this projection is a unital ring homomorphism. Hence
The decomposition matrix separates into two connected components. The first contains and ; it is the principal block . The second contains only and ; since contains the full 5-part of , this is a defect-zero representation and its block has defect group .
For , the normalizer is , so the Brauer correspondence is the identity and corresponds to itself.
The defect group of the principal block is a Sylow 5-subgroup . There are six Sylow 5-subgroups in , so the orbit-stabilizer theorem gives
The centralizer of a 5-cycle in is , and an involution in the normalizer acts on by inversion. Hence
In characteristic five the simple -modules are inflated from : their Brauer characters are and on the identity and involution classes. If are the two one-dimensional and two two-dimensional ordinary characters of , their reductions are
The resulting decomposition matrix is connected, so these characters form the unique 5-block of , with defect group . By the Brauer first main theorem,
This is the complete 5-modular blocks of A5 correspondence.
Let be a projective resolution of the trivial -module. The projective-resolution definition of group cohomology is
This is independent, up to a natural isomorphism, of the chosen projective resolution.
The degreewise natural isomorphisms
commute with the coboundary maps. Taking cohomology proves that group cohomology commutes with finite direct sums:
Now restrict from to a subgroup . The group ring is free as a -module, so restriction carries free modules to free modules and projective modules to projective modules. Thus the restricted complex is a projective resolution of the trivial -module. For the coinduced module , the Hom functor adjunction for a coinduced module gives an isomorphism of cochain complexes
Explicitly, a map is sent to ; the inverse sends a -linear map to . Taking cohomology proves Shapiro's lemma:
For the conjugation module of a group ring , the basis is the disjoint union of its conjugacy classes. Hence is the direct sum of the integral permutation modules on those classes. The class of a representative is the transitive -set , where is its centralizer. Since is finite, this permutation module is both induced and coinduced from the trivial -module . Applying group cohomology commutes with finite direct sums and Shapiro's lemma yields the group cohomology of a conjugation module:
The symmetric group has three conjugacy classes, represented by the identity, a transposition, and a three-cycle. Their centralizers are respectively
For any finite group acting trivially on ,
because a group homomorphism sends an element of finite order to an element of finite order, while the additive group of the integers contains no nonzero torsion elements. Therefore
The periodic resolution of a finite cyclic group alternates the maps and . After applying with the trivial action, these become alternately zero and multiplication by , proving
Combining this calculation with the supplied gives
p-radical subgroup 2026-10-14
A p-subgroup is p-radical if it equals the p-core of its normalizer. Every defect group of a block is p-radical by defect groups are centralizer-conjugate Sylow intersections. Being an intersection of arbitrary Sylow subgroups alone is weaker than the centralizer-conjugate statement used in that argument.