Abelianization Created 2026-09-24 Updated 2026-10-14
The abelianization of a group is the quotient group
where is the commutator subgroup. Its elements are cosets, and its operation is . The result is an abelian group: the two products and differ by a group commutator, which disappears in the quotient group.
For the symmetric group , the sign of a permutation realizes , as shown in commutator subgroup of the symmetric group on three letters. For the dihedral group of a square, abelianization of the square symmetry group gives : two independent yes-or-no pieces of information survive. An abelian group already has , so its abelianization is isomorphic to itself. At the other extreme, a perfect group has trivial abelianization.
Calling this the largest abelian quotient means that every group homomorphism into any abelian group factors uniquely through . It does not require to be finite, or compare the sizes of unrelated abelian groups. The universal property of abelianization makes this precise. It lets us solve all such mapping problems in one simpler group: any invariant that respects multiplication and takes values in an abelian group sees only .
For the symmetric group , take the transpositions and . Products of permutations apply the rightmost factor first. Then
The last permutation sends , , and : two swaps fail to commute by an entire three-cycle.
Figure 1. . The upper rows group the six permutations by sign of a permutation. Each triangle labels the original vertices in their new positions. The lower row applies successively, giving under the rightmost-first convention. The commutator subgroup consists of the three even permutations; the center of a group here contains only . Details.
Every group commutator has sign of a permutation , so , the alternating group of even permutations. Conversely, the displayed group commutator generates . Therefore . The two cosets are the even permutations and the odd permutations, and their multiplication is just multiplication of signs:
This is the first isomorphism theorem applied to the sign of a permutation. Once commutativity is forced, all three transpositions become indistinguishable, and both three-cycles become the identity element. The surviving information is exactly whether the permutation is even or odd. Compare the very different center of a group .
Take the symmetric group and the subgroup of group order two. With the rightmost permutation applied first, its three left cosets are
The subscripts record the image of : every member of sends to . Because is the stabilizer subgroup of in the usual group action, is a bijection onto . It is an equivariant map, since . The coset action therefore becomes the familiar group action on three letters. In particular,
Figure 1.
Three left cosets turn left multiplication in into its faithful group action on three labels
. An original computed coset partition matches each two-element coset to the common image of . The two rows show left multiplication by and . The three stabilizer subgroups intersect only in the identity element. Details.
The three stabilizer subgroups are
Their intersection is , so the subgroup core and the group kernel are trivial. This proves that the coset action is a faithful group action even though every point has a nontrivial stabilizer subgroup. The orbit-stabilizer theorem reads , while the induced group homomorphism gives six distinct permutations of the three cosets. For example, and agree at , but disagree at ; inspecting one label would miss their difference.
The subgroup need not be a normal subgroup for the coset action to exist: . Here the group action is informative because the three conjugate stabilizer subgroups have no common nonidentity element. For the normal subgroup instead, nonfaithful coset action of the symmetric group on three letters shows that only the sign of a permutation survives.
Fermionic time ordering 2026-10-25
For two odd fermionic operators, time ordering contributes a minus sign whenever the chronological rearrangement exchanges them. For several fields the sign is the sign of a permutation restricted to the odd fields. This convention makes the free Dirac propagator a Green function of the Dirac equation with its contact term fixed by the canonical anticommutation relations.
Group homomorphism Created 2026-09-24 Updated 2026-10-14
A group homomorphism is a map preserving the group operation: . It also preserves the identity element and inverse elements. In an additive group, the same requirement reads . A group homomorphism preserves a way of combining inputs, even when several inputs have the same output.
Reduction modulo three from to is a group homomorphism: reducing a sum agrees with adding the reduced residues. For example, modulo six, and both sides reduce to one modulo three; the outputs and also add to one modulo three. This map is surjective but not injective, since zero and three both map to zero.
The sign of a permutation gives another example, from the symmetric group to the multiplicative group . A product of two odd permutations is even, matching . Its group kernel is , the alternating group of even permutations. This shows how a group homomorphism can retain a useful feature while forgetting other details.
Kernel of a group homomorphism Created 2026-09-24 Updated 2026-10-14
The kernel of a group homomorphism is the group version of a kernel. For , it is
It is a normal subgroup of the domain: for in the group kernel, . The group kernel describes inputs whose effect disappears after mapping. For reduction modulo three from , it is ; for the sign of a permutation on , it is . A group homomorphism is injective exactly when its group kernel contains only the identity element.
For indices in , this Levi-Civita symbol is zero when any indices repeat, and otherwise is the sign of a permutation taking to . Thus and exchanging any two index slots changes the sign. It expresses a determinant as with repeated indices summed. Exactly components are nonzero, so .
Let , the symmetric group on three letters, and take the normal subgroup , the alternating group of even permutations. Its two left cosets are
Products of permutations apply the rightmost factor first. Left multiplication by an even permutation preserves both cosets, while left multiplication by an odd permutation exchanges them. For example,
Consequently all six group elements give only two distinct permutations of . Both stabilizer subgroups equal , so their intersection, the group kernel, is . This is a transitive group action because reaches the other coset, but it is not a faithful group action because fixes both.
Figure 1.
A transitive group action of on two cosets detects only the sign of a permutation
. This computed example groups the six permutations by their induced permutations of the two cosets. All three even permutations fix both labels; all three odd permutations exchange them. The group kernel has three elements. Details.
The orbit-stabilizer theorem still works perfectly: . It counts reachable labels, without asserting that the induced group homomorphism is injective. The quotient group captures exactly the two visible operations, identity and exchange. This is the same group homomorphism as the sign of a permutation, with represented by fixing both labels and by exchanging them. Contrast the three-label example in faithful coset action of the symmetric group on three letters.
Normal subgroup Created 2026-09-24 Updated 2026-10-14
A subgroup is a normal subgroup when for every . In other words, conjugation by any group element preserves the subgroup as a set, although it may exchange its individual elements. Equivalently, for every : the left and right cosets of agree. Write .
Every subgroup of an abelian group is a normal subgroup, because conjugation fixes each element. Normality can also hold in a nonabelian group: in , the three even permutations form the alternating group , a normal subgroup as the group kernel of the sign of a permutation. Its two cosets separate the even and odd permutations.
In contrast, is a subgroup of but is not a normal subgroup. With function composition of permutations acting rightmost first, choose . Then
which are different cosets. Also , directly contradicting invariance under conjugation. Thus a subgroup alone does not suffice for quotient group multiplication.
Figure 1.
A normal subgroup gives matching left and right cosets, while a nonnormal subgroup can give different ones
. Details.
The practical value of normality is coset multiplication is well-defined exactly for normal subgroups. Each coset can act as one element of a quotient group, with results independent of representatives. Conversely every normal subgroup is the group kernel of its quotient map of groups, so normality also identifies which distinctions a group homomorphism can consistently forget.
The trivial representation and sign of a permutation give
They are one-dimensional representations, hence irreducible representations. Their characters, in the conjugacy class order of solution, are
These are the only one-dimensional representations. All transpositions are conjugate, so they have the same scalar image in any one-dimensional representation; since a transposition squares to the identity, . Transpositions generate the symmetric group, fixing the whole representation once is chosen.
By the sum of squares of irreducible representation dimensions, the three remaining dimensions satisfy , with each . No can be at least , since . Thus the only possible dimensions are
Use the composition convention . Then . Since the sign of a permutation is multiplicative, the same calculation gives . Both send the identity to and have inverses given by , so both are group representations.
The trace of a permutation matrix counts fixed points, and multiplying that matrix by its sign of a permutation multiplies its trace by that sign. Thus the two characters are
Let and . Both are invariant subspaces, and . On , is the trivial representation and is the sign representation. Subtracting their characters yields
The character inner product verifies that it is an irreducible representation:
The squares of the entries of are identical, so its character inner product with itself is also one. Their values at a transposition differ, so these irreducible representations are inequivalent. Therefore
Alexandre-Théophile Vandermonde presents a programme in elimination theory: remove unknowns from simultaneous polynomial equations in a way that works uniformly as the number of equations and their polynomial degrees vary. The immediate achievement is narrower than that programme: a general construction for linear equations. The academy year 1772 used in the exam is not the printing date of the memoir, which appeared in 1776. Its compact indices distinguished the equation containing a coefficient from the unknown it multiplied; they were not powers. That notational separation is crucial to interpreting the work.[ref][ref]
In modern language take a system of linear equations with unknowns. Its determinant is an alternating expression in the coefficients:
Each product selects one coefficient from each equation and each unknown's column. The sign of a permutation determines whether it is added or subtracted. This makes the number a genuine parameter of a general rule, rather than merely supplying separately memorised formulas for two or three unknowns. The notation here is modern, not a transcription of Alexandre-Théophile Vandermonde's symbols.
For two unknowns, multiply by and by , then subtract. Similarly eliminate . This gives
The same principle in arbitrary size is Cramer's rule. If is obtained by replacing column of by , then
An original verification uses the multilinearity of the determinant: replace by the column combination . Every resulting determinant vanishes through repeated columns except the term, which is . This explains how an elimination expression isolates one unknown.
The condition is substantive. If , multiplying by an expression which vanishes cannot justify division. For instance, and are inconsistent, whereas replacing by gives infinitely many solutions. Thus an elimination formula must distinguish exceptional coefficients and preserve the connection to the original system of linear equations. Nor does the displayed rule solve the much broader problem of arbitrary nonlinear equations.
The passage's importance is the move from particular elimination calculations towards a theory of alternating expressions. It would be misleading to turn this into the claim that the familiar Vandermonde determinant, formed from powers of variables, is what this extract displays. A positional upper index and an exponent have different meanings; the history of that eponym requires separate evidence. Likewise, modern matrix algebra is a useful explanatory language here, not the institutional or conceptual setting of an eighteenth-century memoir.[ref]
In components the scalar triple product is . A cyclic permutation has positive sign of a permutation, so . Relabelling the summed indices therefore gives
which proves . Equivalently both expressions are the same three-column determinant.
Reversal has one inversion of a permutation for every pair of indices, hence inversions of a permutation. The sign of a permutation gives
It is for and for .
The determinant is unchanged by transposition: . In the Leibniz formula for determinants, replacing each permutation by its inverse interchanges the row and column roles without changing its sign of a permutation.
Compose permutations from right to left. Tracking the four symbols through the two permutation cycles gives and . Thus the cycle decomposition of a permutation is
The disjoint transpositions commute, and squaring their product gives the identity element, while the product itself is nonidentity. Its order of a group element is therefore two. Each transposition has negative sign of a permutation, so the product has sign : it is an even permutation.
If , cancellation of successive factors gives for every positive integer . Hence is the identity element exactly when is, proving that conjugate group elements have the same order of a group element. For permutations, the sign group homomorphism similarly gives
Thus conjugate permutations have the same sign of a permutation.
The converse is false: permutation order and sign do not determine conjugacy. In the symmetric group , take and . Both have order three and positive sign. However, fixes three symbols whereas fixes none. If fixes a symbol , then fixes , and applying the inverse conjugation gives a bijection between the fixed-symbol sets. Their different fixed-point counts therefore prove that are not conjugate. Equivalently their cycle types and differ. Equal order and sign are necessary, but not sufficient, for conjugacy.
Use the Leibniz definition of the determinant:
For the permuted-column matrix, . Reindex the sum by . The sign of a permutation is multiplicative, so . It follows directly that
For the matrix transpose, the products in its determinant are . Set to obtain , and use . This proves . These facts also show that equal columns, or equal rows by transposition, force the determinant to be zero: exchanging the equal pair leaves the matrix unchanged but changes the determinant's sign.
Let be the matrix obtained by deleting row and column , with the empty determinant taken as one for . Define the cofactor and the adjugate matrix by . Grouping the Leibniz sum according to the column chosen in row gives the cofactor expansion : deleting that row and its chosen column leaves a permutation of entries, with sign factor . Therefore
When this is . When it is the cofactor expansion along row of the matrix formed by replacing that row with row ; its remaining minors are unchanged, and its two equal rows give determinant zero. The column version proves the other product in the same way. Thus the adjugate identity is
For the real matrices , let . The determinant definition makes this a real polynomial of degree of a polynomial at most . Since is invertible, the allowed converse implies , so is not the zero polynomial. It has at most real roots of a polynomial. Choose a real outside those roots; the adjugate argument proves that is invertible.
Finally write the given complex similarity transformation as . The relation , with real, yields and by comparing real and imaginary parts. Choose the preceding and put . Then , so
This proves real similarity from complex similarity by constructing a real intertwiner, rather than requiring or separately to be invertible.
Work with finite groups, as required for these Sylow subgroup counts. Let act by conjugation on the set of Sylow -subgroups. The stabilizer of is . Since is the normal Sylow subgroup of its own normalizer, every -subgroup of that normalizer lies in . Consequently the stabilizer is exactly , and the orbit-stabilizer theorem gives orbit size . The orbit of has size one. Every other orbit size is a power of at least , hence is divisible by . Adding orbit sizes proves the strengthened Sylow congruence from intersections:
Now suppose is simple of order . If , its Sylow -subgroup is normal because its number divides three and is one modulo five. If , an involution in the regular permutation action of swaps fifteen pairs, so its sign is negative. The sign of a permutation would give a nontrivial group homomorphism with a proper nontrivial normal kernel. Both cases contradict simplicity. Thus .
The Sylow theorems make a divisor of fifteen. It is not one, since a nontrivial Sylow subgroup would then be normal. It is not three, since the conjugation action on three Sylow subgroups would give a faithful group homomorphism , impossible by order. If , take a Sylow subgroup itself: its normalizer has subgroup index five. If , not all distinct Sylow subgroups can intersect in subgroup index at least four, since that would give . Choose with . Put , of order . It has subgroup index two in both , so is normal in each. Hence contains both distinct Sylow subgroups and has order greater than . It is proper: otherwise would be a nontrivial proper normal subgroup of . Its order is therefore or . The latter would give an index-three subgroup and again an impossible faithful action on three cosets. Thus .
In either case we have the requested subgroup of order or with index-five normalizer. The action on the five cosets of that normalizer is nontrivial and faithful by simplicity. Its image lies in , since composing with sign cannot give a nontrivial map from this simple group of order greater than two to . Thus divides , forcing and equality of orders. This proves the simple groups with order a power of two times fifteen conclusion:
For , choose the first column: there are nonzero choices. For each, determinant one is a nonzero linear equation in the second column and has five solutions. Therefore . A central matrix commuting with has zero lower-left entry and equal diagonal entries; commuting also with makes the upper-right entry zero. It is scalar. Determinant one then gives
To establish the projective special linear group over the field with five elements isomorphism without assuming its simplicity, compute its classes. For determinant-one matrices, the characteristic polynomial is with trace . The possibilities over exhaust the group:
For trace zero the eigenvalues are , so the determinant-one centralizer is the split diagonal torus of order four. For traces , the discriminant is the nonsquare : the centralizer is the norm-one subgroup of , of order six. In both semisimple cases the determinant map on the full linear centralizer is surjective onto ; consequently each trace type is a single special-linear class. For the noncentral traces , a Jordan block has full linear centralizer with determinant . The determinant image consists of the two squares, so each general-linear class splits into two special-linear classes; the determinant-one centralizer has order . These sizes sum to .
Quotienting by identifies a matrix with its negative. The trace-zero class gives one projective class of size fifteen; the two traces give one class of size twenty; the four noncentral unipotent classes give two classes of size twelve. Their respective projective orders are , by the characteristic polynomials. A normal subgroup is a union of classes containing the identity. The nontrivial proper possible union sizes are , none of which divides . Thus the quotient is simple. Applying the order- result above gives
Finally, if over an odd-characteristic field, its minimal polynomial divides the square-free polynomial , so it is diagonalizable with eigenvalues . In dimension two, determinant one requires both eigenvalues equal. Hence or . This proves the unique involution in SL2 over an odd field assertion: the only element of order two in is . If an index-two subgroup existed, it would be normal and have order sixty. By Cauchy theorem it would contain an involution, hence contain . Then would be a normal subgroup of order thirty in the simple quotient , a contradiction. Thus has no index-two subgroup.
Compose permutations from right to left. Tracking the images gives , , and , so
Two transpositions give sign of a permutation , proving that this element belongs to the alternating group .
Its conjugacy class consists of all double transpositions. Conjugation merely relabels the letters, so no other cycle type can occur. Conversely, choose a permutation relabelling the two pairs into any desired two pairs. If is odd, replace it by : the transposition centralizes , so this replacement is even and gives the same conjugate. Thus every double transposition is reached by conjugation inside .
The complete list of fifteen elements, grouped by their fixed letter, is
There are five choices of fixed letter and three pairings of the other four letters, confirming the conjugacy class size .