Given a prime factorization , repeatedly apply part (c) to the cyclic group of order : it has a chain of subgroups of successive orders
Read in increasing order, this is a composition series with factors isomorphic to the cyclic groups of orders . Any second prime factorization of the same integer produces another composition series of the same group .
The Jordan–Hölder theorem equates the two multisets of simple factors. Since for primes implies by equality of group orders, the two prime multisets agree. Hence
For both factor lists are empty, corresponding to the trivial group.
The exact orders printed in the question are inconsistent. The source PDF says that the orders of group elements are , respectively, and also imposes . Multiplying this relation by and using gives . Since also holds, subtracting gives , contradicting the stated order of a group element . Thus
The natural abelian group presentation interpretation is to impose the relations and , with no further relations, without requiring the orders of the images of the generators to stay . Under this interpretation the calculation is as follows. Since follows from , the mixed relation gives . Consequently , and together with this gives . Conversely, , , and imply every original relation. Eliminating leaves two independent cyclic groups:
To verify that these relations force no further identifications, map to in . All defining relations hold, and the inverse group homomorphism sends the two standard generators to . These group homomorphisms are mutually inverse. The divisibility condition gives the requested invariant factors of a finitely generated module over . In this presented group, actually have orders .
Equivalently, the relation matrix
has nonzero Smith normal form entries , with the trivial factor omitted. The displayed direct sum of modules is the answer to the presentation interpretation; the inconsistency of the literal exact-order formulation remains.
Write . The unit group is a finite abelian group of group order , since multiplication in a field satisfies commutativity. The structure theorem for finitely generated abelian groups, applied to this finite group, gives invariant factors of a finitely generated module
after omitting trivial factors. If there are no factors, the unit group is trivial and hence a cyclic group.
Otherwise put . Every element satisfies , because the order of a group element in each coordinate divides . Hence all distinct nonzero elements of are roots of a polynomial . The root bound for a polynomial over a field gives
For completeness, that bound follows by induction from the factor theorem: if a nonzero polynomial vanishes at , write ; every other root of a polynomial is a root of , because a field has no zero divisors. Each new distinct root therefore uses one unit of polynomial degree.
On the other hand, the group order in the decomposition is
Equality is forced, so . As every retained factor is greater than , there can be only one. Consequently
The same proof establishes the more general result finite multiplicative subgroup of a field is cyclic. The square-free integer result in part (c)(i) alone would not suffice, since need not be a square-free integer; the root bound for a polynomial rules out multiple invariant factors of a finitely generated module even then.
Let be a square-free integer. If , then is the trivial cyclic group. Otherwise, finiteness means that a direct sum of modules decomposition into cyclic groups has only finitely many nontrivial factors, each of finite group order. Omit trivial factors and write
The integers are coprime integers whenever . If a prime number divided both, then , contradicting the square-free integer hypothesis.
Moreover, and are coprime integers: any common prime divisor would divide one of the earlier factors as well as . Thus part (b)(ii) can be applied repeatedly to combine factors, giving
In particular is a cyclic group. Under the displayed identifications, the element whose coordinate in every factor is the class of is a generator of a group.
Choose a generator of the cyclic group , so . Part (a)(iii) gives a unital ring homomorphism . Its image lies in the centre of , so even if is not a commutative ring, evaluating a polynomial at defines a ring homomorphism
Because , it factors through the quotient ring to give
Its image is the subring . Every unit of is a unit of , because an inverse in also lies in . Conversely, every member of is for some , and both and its inverse lie in . Hence
The inverse argument matters: merely belonging to a subring would not by itself make an ambient unit invertible there.
A simple group is a nontrivial group whose only normal subgroups are itself and the trivial subgroup.
A composition series is a chain in which each is a normal subgroup of and each quotient group is simple and nontrivial. Its length is , and these quotients are its composition factors. The individual terms need not all be normal in .
A solvable group is a group whose derived series reaches the trivial group: starting with , define . For finite groups this is equivalent to having a composition series whose factors are all cyclic groups of prime order.
The Sylow theorems also give and . Of , only is congruent to one modulo five. Thus is a normal subgroup of as well.
By Lagrange's theorem, , since its group order divides both and . For and , the group commutator lies in by the normal subgroup property of , and in by the normal subgroup property of . It is therefore the identity element, so all elements of commute with all elements of . This is the fact that normal subgroups of coprime order commute.
The subgroup consequently has elements: the expression is unique because . Since and have prime orders, they are cyclic groups. Write and . The product of commuting elements of coprime order has order , so generates . Finally, is a normal subgroup because both its factors are normal subgroups; equivalently, it has subgroup index two. Therefore
Let . The allowed center of a group theorem gives . By Lagrange's theorem its order is or . In the first case has order and is a cyclic group. A cyclic quotient by the center forces to be Abelian: if , write arbitrary elements as with , and commute them directly. Hence in every case
For two examples at prime-cube order, take the dihedral group of a square, , and the quaternion group . Both have order . They are nonabelian because and , respectively. They are distinct examples even up to group isomorphism: the dihedral group has five elements of order two and the quaternion group has only one. The request asks for two examples; it does not require the prime to be arbitrary.
The Abelian group criterion for a product of two prime squares applies because and . Here its Sylow theorems proof is especially short:
The candidates for are , of which only has the required remainder. The candidates for are , again leaving only . Thus both Sylow subgroups are normal subgroups. Their group commutators lie in , and , so . Both factors are abelian groups of prime-square order by (a).
The Fundamental theorem of finitely generated abelian groups gives precisely
These four groups are pairwise nonisomorphic: their characteristic Sylow subgroups differ in whether they contain an element of order or . The first is also the cyclic group .
The multiplicative group is a cyclic group of order , so choose a primitive root . Every nonzero residue is uniquely , with taken modulo . The condition becomes . Writing , its solutions are . Zero is not a solution. Therefore the number is
This includes . The cyclic group argument gives the exact count, whereas the bound of roots for a nonzero degree- polynomial over a field would only give an upper bound.
There are six functions: the four power maps for , and the two constant maps . All calculations in this part are in the finite field .
Put . Multiplicativity gives , so the absence of zero divisors forces or . If , then for every , giving only the constant-zero map.
Suppose . For nonzero , the equality shows . The nonzero elements form a cyclic group generated by , in the order . Choosing determines every value on this group by . Each satisfies , so all four choices give consistent group homomorphisms.
Finally, satisfies and for every . The choice works for all four group maps. The choice forces every nonzero value to be , giving one extra map, the constant-one map. Thus the count is . The four zero-preserving possibilities are exactly the four displayed power maps. This is the special case with five elements of multiplicative self-maps of a finite field.
A group is poly-(cyclic or finite) when it has a finite subnormal series in which each quotient is a cyclic group or a finite group. Each term need only be normal in the next term. The polycyclic group condition instead requires every factor to be cyclic.
The scalar sign action of a cyclic group of order two on has invariant ring . It is not factorial: are pairwise nonassociate irreducibles, since every nonconstant invariant has degree at least two, while gives two distinct factorizations.
Let be the plane rotation matrix through , generating a cyclic group of order four. A quadratic form has its two coefficients exchanged by a quarter-turn and unchanged by a half-turn. Thus the pullback action on this two-dimensional space gives the displayed group representation: , with . It is not a faithful representation, because its kernel of a group homomorphism is . Its two invariant coefficient lines correspond to and , on which a quarter-turn acts by and , respectively. Restricting to this diagonal space is valid for these signed coordinate permutations; a general linear transformation can introduce an term.
Quotient group Created 2026-09-24 Updated 2026-10-14
For a group and a normal subgroup , the quotient group is the set of cosets , with operation
Its identity element is the coset , and the inverse element of is . A quotient group treats all elements within one coset as the same input while retaining a consistent operation on the classes. The normal subgroup condition is what makes this operation independent of which representatives are chosen. [ref].
Take the additive group and . Since is an abelian group, is a normal subgroup. There are three elements in the quotient group:
Adding two copies of gives ; adding and gives . Hence the quotient group has the addition table of . It does not select one representative and discard the others: its elements are the entire cosets.
Figure 1.
Identifying residues differing by three turns a six-element cyclic group into a three-element quotient group
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This is useful whenever distinctions within a normal subgroup should be ignored. For example, the sign of a permutation retains only even or odd parity of a permutation in . Its group kernel is the alternating group , and the quotient group has two elements. The first isomorphism theorem explains why a group homomorphism's image is a quotient group of its domain.
Quotient set Created 2026-09-28 Updated 2026-10-14
A quotient set packages each equivalence class as a single new set element. It remembers which class an original set element belongs to and forgets which member of that class it was. For an equivalence relation on a set ,
Each set element of the quotient set is itself a nonempty subset of . The canonical projection of a quotient set sends an original set element to this entire equivalence class. [ref]
For integer congruence modulo three restricted to , the quotient set is
It has cardinality three. The set is a choice of equivalence class representatives, not literally this quotient set: is an integer, while is a set. The function sending each chosen equivalence class representative to its equivalence class is a bijection between these two different sets.
Figure 1.
The quotient projection sends nine elements to three classes, with each class appearing as one fiber
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A quotient set alone specifies no arithmetic. To obtain the familiar modular arithmetic example with addition, use integer congruence on the whole set of integers. Its quotient set is , where is an infinite residue class. Define addition by
The answer must be independent of the equivalence class representatives. If and , then , so both sums have the same residue class. This is what it means for the group operation to be well-defined. With this addition, the quotient set is a cyclic group, with identity and inverse for . [ref]
For example, . Choosing and as different representatives of an equivalence class for gives the same sum; choosing and gives again. These calculations use residue classes of all integers. Raw addition on the finite does not stay in : . The formula for addition on therefore cannot be applied as a raw inherited operation on that finite example.
Representation theory Created 2026-09-24 Updated 2026-10-20
Representation theory describes abstract symmetries by linear maps on vector spaces. A group representation assigns an invertible linear map to each group element, respecting multiplication. The payoff is that a symmetry problem becomes a problem about matrices, invariant subspaces, and eigenvalues. Decomposing the action can reveal combinations of variables that a symmetric system cannot mix.
Take the cyclic group , with . On three real coordinates, let send to :
This permutation representation does more than relabel a list: it acts linearly on every possible assignment of values to the three positions. The vector stays fixed. The vector subspace is also preserved, since a permutation does not change the sum.
Every vector separates uniquely into these two types:
For example, . The first term belongs to a trivial representation; the second is a contrast with zero coordinate sum. This is a direct sum decomposition . The symmetry preserves the mean and rotates the contrasts.
Figure 1.
Three-coordinate cyclic symmetry preserves the mean and rotates the zero-sum contrasts by 120 degrees
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The rotation is literal after choosing the orthonormal basis , of . In this basis,
It is a rotation through degrees, and three applications return to the starting point. There is no nonzero invariant real line, because this rotation has no real eigenvector. Thus the two-dimensional action is an irreducible representation over the real numbers. Over the complex numbers it instead splits into two eigenlines with eigenvalues and . The coefficient field is part of an irreducibility claim.
Why would this decomposition matter for a physical calculation? Consider three equal masses with scalar displacements and the symmetric quadratic coupling energy
The equations of motion are , where
is a graph Laplacian and is the all-ones matrix. The constant vector has eigenvalue zero: translating all coordinates equally costs no coupling energy. On , vanishes and , so both independent contrast directions have angular frequency . A three-coordinate coupled problem reduces to a free mean and two identical harmonic oscillators.
Figure 2.
Equal pair couplings leave the mean fixed and make two independent zero-sum modes oscillate at the same frequency
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For initial displacement and initial velocity zero, the exact solution is . The fixed mean and oscillating contrast can be read directly from the decomposition. More generally, a linear operator commuting with the group action carries its fixed-vector subspace into itself; with an invariant inner product, it preserves the corresponding orthogonal complement too.
For a finite group, averaging over the action constructs an invariant inner product over the real numbers or complex numbers. The resulting invariant complements explain Maschke's theorem: a finite-dimensional group representation decomposes into irreducible representations. Characters compress the action into traces and help identify those pieces. The assumptions matter; in modular representation theory the coefficient field can have characteristic dividing the group order, and such decompositions can fail. Chapter 4 of Pavel Etingof and coauthors' notes develops these mechanisms. [ref].
These roots are taken in an algebraic closure, not merely in . If the characteristic of a field is and with , then ; hence there are distinct roots. They form a cyclic group by the finite multiplicative subgroup of a field is cyclic theorem. In particular they have order when .
A group action on a nonempty set is simply transitive when exactly one group element sends any chosen point to any other:
Equivalently it is both a transitive group action and a free group action; this is also a regular group action. Transitivity supplies a transport, and freeness makes it unique. Conversely, putting in the uniqueness condition shows that every stabilizer subgroup is , since the identity element already fixes . In a transitive group action, checking that just one stabilizer subgroup is trivial suffices: all the others are conjugate subgroups.
The cyclic group in the diagram under transitive group action is simply transitive. More generally, the left regular action of any group on itself is simply transitive: the equation has the unique solution , using the inverse element of . This shows why the property is useful: every position has a unique label relative to a chosen starting position.
Choose a point . Its orbit map
is a bijection and an equivariant map from the left regular action: . This identifies with a copy of , but does not come with a preferred identity element. If , then : changing the chosen point composes this identification with right multiplication by . An old label therefore becomes the new label , which also specifies the side of multiplication for a noncommutative group.
The transport from to remains independent of the chosen point. Writing and , it is . With , the new labels are and , and
For a finite group, simple transitivity implies . Conversely, a transitive group action with is simply transitive by the orbit-stabilizer theorem. Equality of cardinalities alone is insufficient without transitivity: the cyclic group can fix both points of a two-point set, giving two group orbits and two possible self-transports at each point.
Stabilizer subgroup Created 2026-09-24 Updated 2026-10-14
For a group action of a group on a set , the stabilizer subgroup of consists of the transformations that leave fixed:
It is a subgroup: the identity element fixes , products of transformations fixing fix , and the inverse element of a transformation fixing also fixes . A stabilizer subgroup is a subset of , whereas the orbit of a group action is a subset of . See Ackerman's algebra notes, definition 0.4.1.2.
For the square group actions defined under group action, direct calculation gives
The reflection fixes and individually. The reflection preserves the unoriented side of a polygon by exchanging its two vertices of a polygon. The half-turn rotation exchanges the two ends of the unoriented diagonal of a polygon while preserving that diagonal of a polygon. Thus fixing a side of a polygon or diagonal of a polygon as an object does not mean fixing every point on it; the latter condition uses a pointwise stabilizer. The four stabilizer subgroups have group orders , matching group orbit sizes through the orbit-stabilizer theorem.
A stabilizer subgroup records the transformations still available after imposing a constraint. Fixing a vertex of a polygon of the square leaves two choices; fixing its centroid leaves all eight. In a faithful group action, a stabilizer subgroup can still contain a nonidentity transformation, as shows: a faithful group action requires that only the identity element fix every point of simultaneously, not that every individual stabilizer subgroup be trivial. The two-point cyclic group example under group action has both stabilizer subgroups equal to the group kernel of its associated group homomorphism.