If is the character of , then Burnside lemma applied to the diagonal action on gives
For a transitive action , this also equals the number of double cosets in .
For the order-eight dihedral group generated by of order four and of order two with , let . There are exactly three double cosets: , , and , of sizes two, two, and four. Their number does not divide eight. This differs from the number of ordinary cosets, which divides group order by Lagrange's theorem.
Double-coset Hecke algebra Created 2026-10-05 Updated 2026-10-06
For a group and subgroup such that every double coset has finitely many orbits under left multiplication by , this algebra consists of complex -bi-invariant functions on supported on finitely many double cosets. Its convolution is
The double coset indicator functions form a basis. On invariant modular functions it acts on the right by . For and , rational conjugation of finite-index modular subgroups verifies the finiteness condition. The determinant- Hecke operator uses the indicator of all integral determinant- matrices, not only a single double coset when is composite.
A double coset is generally not a subgroup, so Lagrange's theorem does not force its size to divide the ambient group order. In , take . Then has size two, while has size four, which does not divide six. The general size formula explains why different double cosets can have different sizes.
Use finite-dimensional -modules or finite -free lattices. We use the basic relative-projectivity facts that Krull-Schmidt decomposition holds with local endomorphism rings, module vertices are conjugate p-subgroups, and a module source at a module vertex satisfies and . Module induction is transitive and Mackey restriction formula gives module vertex containment for restrictions and inductions. In particular, a summand induced from has module vertex conjugate into , and module restriction to a subgroup containing a chosen module vertex retains a summand with that module vertex. The latter follows from the module source conditions and minimality: restricting further to must still contain its module source, whose module vertex is .
The module vertex- form of Green correspondence states that for there is a bijection between indecomposable -modules with module vertex and indecomposable -modules with module vertex . Its maps select the unique module vertex- summands of module restriction and induction, using -conjugacy for restricted module vertices and -conjugacy for induced module vertices. They occur with multiplicity one and have the same module sources. Other induction summands have module vertices conjugate to proper subgroups of . The module restriction remainder is relatively projective for
Relative projectivity for a family means being a summand of a finite sum of inductions from its members. We prove this form; no stronger description of the induction remainder is needed for the application.
Let have module vertex over . The identity double coset in Mackey restriction formula gives
Since is relatively -projective, a further Mackey decomposition puts every other double coset term in the relatively- family. No member of contains an -conjugate of . Otherwise, conjugation within would give with , . Equality of orders then makes , a contradiction. Therefore the module restriction above contains exactly one summand with module vertex -conjugate to , namely once.
Decompose into indecomposable modules. All their module vertices are conjugate into . Each one with a module vertex -conjugate to can take itself as module vertex and contributes a module vertex- summand on module restriction to . There can thus be at most one such summand and its multiplicity is one. There must be at least one, because smaller module vertices cannot restrict to produce , with module vertex , in the displayed decomposition. Define to be that summand. Its module restriction contains once, with remainder a summand of . All other induction summands have strictly smaller module vertices. This is Green correspondence from Mackey multiplicity.
Conversely take of module vertex over with module source . Decompose into indecomposable modules. Since , the local endomorphism ring and Krull-Schmidt decomposition give for one indecomposable summand of . Its module vertex is -conjugate to : all module vertices are conjugate into , and a smaller one could not induce . The preceding uniqueness makes and identifies as the unique module vertex- summand of . Define . This proves and .
If is a module source of , then and . These two conditions and the common module vertex show that is also a module source of . Thus the correspondence preserves module sources, including trivial source modules, and the proof is complete under the stated coefficient conventions.
For the required expression, a p-local module is a finite sum of inductions from for nontrivial p-subgroups . Induct on the order of a module vertex of . Vertex 1 makes projective, so choose , .
For module vertex , take for . Its module induction is p-local and
with smaller module vertices for the . By induction, write
with p-local and projective. Adding these identities and substituting the induction decomposition gives
Hence the explicit choices
work. All sums are finite and module vertex orders strictly decrease, so the induction terminates. If , induction from that normalizer is still allowed by the definition of p-local.
Write for the two given congruence subgroups, to distinguish them from the notation . Their double coset has a finite decomposition
Finiteness follows because has finite index in . To check this without assuming integrality of , clear its denominators: a sufficiently deep principal congruence subgroup lies both in and, after conjugation by , in . Representatives for give the displayed decomposition.
Using the Hecke-normalized rational slash operator from the PDF, define the double-coset operator on modular forms by
Replacing by for changes no term because . Right multiplication by permutes these left cosets, so . Each summand is holomorphic in the complex upper half-plane. At any rational modular cusp, factor with and upper triangular of positive slope, as in 2(i). The cusp expansion of has no negative terms, and substitution by preserves boundedness. The sum is periodic in a cusp coordinate for , so it has a removable singularity there. This proves
If vanishes at all its cusps, the same argument gives vanishing for the image too.
Now set . For an integer prime to , choose with lower-right entry congruent to modulo . Such a lift exists by choosing with and using . The subgroup is normal in , and its quotient is through the lower-right entry. Define the diamond operator by
Different lifts differ by a member of , so this is well defined. The diamond operators satisfy .
For a prime , put and define the Hecke operator
Choose with and set . A complete set of left-coset representatives is
Here and , with both right factors in . To prove completeness, consists of the members of whose upper-right entry is divisible by . Reduction of modulo is onto : use the Chinese remainder theorem to impose identity modulo and any chosen determinant-one matrix modulo , then lift to by elementary matrices. Reduction of is the lower triangular subgroup. Its left cosets correspond to the lines of top rows in . The right factors give lines , while the last factor gives with . They are all the lines, proving the decomposition.
The printed slash normalization now gives and
Thus
To prove commutation, use the marked-lattice model of a modular form. A pair consists of a lattice and a point of exact order modulo , and a weight- function satisfies . In a basis with , it represents . The diamond operator multiplies by . The same Hecke operator is
Every marked point retains exact order : multiplication by is invertible on its cyclic group, since . This lattice sum agrees with the displayed slash sum. Its overlattices with basis give the first terms, and the remaining one with basis has normalized marked point , giving . Multiplying the mark by commutes with passage to each overlattice and does not change the set of overlattices. Hence
Finally write . The first term of contains the finite average
It therefore contributes to the coefficient of . The second term contributes if , and zero otherwise. This proves the good-prime and bad-prime Hecke coefficient formula at a good prime, without assuming that has a particular character:
where a nonintegral coefficient index means zero. For both terms are retained. On a diamond-character eigenspace the second term becomes .
Throughout, modules are finite-dimensional over , or finitely generated -free lattices when the coefficient ring is . The p-modular system has a complete discrete valuation ring , maximal ideal , fraction field of characteristic zero and residue field of characteristic .
A block of a group algebra is a nonzero, indecomposable two-sided ideal direct summand of . Equivalently it is for a primitive central idempotent . To see the equivalence, suppose as two-sided ideals and write with , . Products between and vanish because they lie in their zero intersection. Thus is the identity on , zero on , and is a central idempotent, with . Conversely . Splitting further is equivalent to splitting into orthogonal nonzero central idempotents; indecomposability is exactly primitivity. If is the block decomposition, . A nonzero indecomposable module therefore belongs to exactly one block of a group algebra, namely the one with .
For modular reduction of block idempotents, the conjugacy class sums are an -basis of . Hence . In the complete commutative algebra , idempotent lifting gives a unique lift of each idempotent of ; uniqueness follows because commuting idempotents congruent modulo the Jacobson radical are equal. Orthogonal decompositions lift too, so primitivity is preserved. Reduction gives a bijection between the integral and modular blocks.
Here is a definition of defect groups of a block which also proves the required relative-projectivity assertion. Give its conjugation action and, for , define the relative trace and its transfer ideal of conjugation-fixed elements by
A defect group of a block is a -subgroup minimal with . Such a subgroup exists: for a Sylow subgroup , is a unit in and . The defect of a block is where .
For completeness, this definition is independent of a choice up to conjugacy. Multiplying two relative traces and grouping the pairs of cosets by double cosets gives
This identity follows by writing each pair of cosets as a simultaneous -orbit; its stabilizer is , and its contribution is a trace from that stabilizer. If are both minimal for , then belongs to the displayed sum. The commutative block center is a local ring: in the field case it is a commutative Artinian ring with no nontrivial idempotents; in the integral case its reduction has this property and completeness detects units. A sum of proper ideals cannot contain its identity. Consequently for some , forcing by minimality. The same argument with an arbitrary shows that precisely when contains a conjugate of . This is the trace criterion for defect groups.
To relate this to the usual modular definition, the Brauer morphism deletes the coefficients outside the centralizer:
It is an algebra homomorphism: in the coefficient of an element centralizing in a product, acts on the contributing pairs; nonfixed orbits have size divisible by , while fixed pairs have both entries in . Its kernel is the sum of proper-subgroup transfers, because the nonfixed conjugation orbit sums form a basis of that kernel. If is minimal for and , replace by . The kernel description gives , contradicting the local-center argument. Also unless is conjugate into : group the cosets of into -orbits, which have no fixed point otherwise. Thus the minimal transfer subgroups are exactly the maximal -subgroups with nonzero Brauer morphism of .
Now take and write . Multiplication by is a -linear endomorphism of , and
Here is the splitting behind the D. Higman criterion. The natural map , , has a -linear section
Changing a representative by an element of leaves this tensor unchanged, permutes the terms, and . Hence
This is relative projectivity for , proving the Green relative projectivity theorem; indecomposability was needed only to speak of a single block of a group algebra or vertex of an indecomposable module.
Finally let lift . A trace expression for reduces to one for , so a modular defect group of a block is contained, up to conjugacy, in an integral one. Conversely choose a modular defect group and with . Conjugation orbit sums lift to . The element
reduces to its block identity, hence is a unit in that block center. Its inverse there is central, so
The integral defect is therefore contained in the modular one. The corresponding blocks have the same conjugacy class of defect groups and the same defect.
The block statement is Green correspondence for blocks: if , blocks of and with defect group correspond, and their block bimodules are Green correspondents for the diagonal vertex . We prove the module correspondence underlying this statement, then specialize it to the block bimodules. This also gives the requested direct proof in the trivial-intersection situation.
Here are the elementary ingredients, including their proofs. Mackey decomposition is obtained by partitioning the tensor basis of by the double cosets ; the term for is induction from of the suitably conjugated restriction of . The D. Higman criterion follows from the section constructed in Question 1. Conversely, take a splitting of the induction counit and its coefficient at the identity coset: equivariance reconstructs the section from that -linear coefficient, and the splitting identity is exactly that its relative trace is . Thus the trace criterion is an equivalence.
An indecomposable module here has a local endomorphism ring. Over this follows from the Fitting lemma: an endomorphism eventually splits its kernel from its image, and indecomposability makes it invertible or nilpotent. Over , the endomorphism ring is finite over a complete discrete valuation ring; lift orthogonal idempotents from its finite-dimensional residue algebra to see that an indecomposable lattice has a local endomorphism ring too. The Krull–Schmidt theorem follows by the usual exchange argument: composing the inclusion and projection of one indecomposable summand across a second decomposition writes its identity as a sum of endomorphisms; one is a unit in the local endomorphism ring and pairs that summand with a summand of the second decomposition. Remove the pair and continue. Existence follows by successively splitting nontrivial idempotents, which decreases dimension or rank.
A vertex of an indecomposable module is a subgroup minimal for relative projectivity. It can be taken to be a -subgroup because averaging over the index of a Sylow subgroup of any candidate subgroup is invertible. If an indecomposable module is relatively projective for and , the Mackey decomposition and its induction splittings make it a summand of a sum of modules induced from . In its local endomorphism ring one splitting component must be invertible, so it is relatively projective for one of these intersections. This proves conjugacy of minimal vertices and the useful criterion that a module with vertex can be relatively projective for only when is conjugate into . A source of an indecomposable module with vertex is an indecomposable summand of its restriction to from which the original module is an induced summand. Such a summand exists by the induction splitting and Krull–Schmidt theorem; its vertex is , since a proper vertex would make the original module relatively projective for a proper subgroup of .
Set
When saying a module is - or -projective, allow conjugates in the relevant ambient group and finite sums of modules relatively projective for members of that family. No conjugate of inside belongs to : if , equality of orders gives , so , contradicting . Every member of is a proper subgroup of .
The two key assertions can now be proved rather than assumed. First, if is an indecomposable -projective -module, then
Choose with . Mackey decomposition gives , with -projective. Write and apply induction and restriction. Both and contain their original modules, by the identity double coset. Comparing multiplicities of every indecomposable which is not -projective, their extra multiplicities are nonnegative and have sum zero. Therefore neither has such an extra summand, proving the assertion.
Second, suppose has vertex , and choose an indecomposable whose restriction contains ; such a exists by the first assertion. Write . Its restriction has just one summand isomorphic to and all other summands are -projective, so is -projective. Any indecomposable has a vertex after conjugacy. A source with vertex is a summand of . Restricting a -projective decomposition of to and using Mackey decomposition forces to lie in an -conjugate of some , . Since , this puts in . Thus is -projective. Moreover has vertex , since it is -projective and its restriction contains with vertex . We have proved
In particular is unique.
Conversely, let be an indecomposable -module with vertex and source . Decompose and choose whose induction contains . Its vertex is contained in and cannot be proper, since induction would then make relatively projective for a smaller subgroup. Thus has vertex , and the previous assertion makes its unique vertex- induced summand. Restriction of an -projective module is -projective: in a Mackey term a conjugating element inside preserves the containment in an -conjugate of , and one outside gives a subgroup of . Comparing the two decompositions of now gives
These assignments are mutually inverse. To check sources, restrict back to . Its terms of full vertex are conjugates of by ; the other terms are induced from proper intersections. Applying the source criterion and Krull–Schmidt theorem shows that the source of is one of those conjugates. The same argument in , and the uniqueness just proved, matches the source classes on the two sides. Thus Green correspondence preserves sources up to normalizer conjugacy.
To pass to blocks of a group algebra, regard as the permutation module . A summand of a permutation module has trivial source. Here is why: over a finite p-group, every transitive permutation module is indecomposable, since its socle is the one-dimensional fixed line and every nonzero module has nonzero fixed points. The latter follows by induction on the group order, using a central element of order and the nilpotence of its difference from . Over indecomposability follows by reduction. Restrict a permutation summand to a vertex and apply Krull–Schmidt theorem; a source must be a transitive permutation module . Its vertex is contained in , so minimality forces , and its source is the trivial module.
For a permutation module, its Brauer quotient of a module at has the fixed permutation points as basis: every nontrivial orbit sum is a proper transfer. An indecomposable trivial-source summand with vertex has nonzero quotient only at subgroups conjugate into , by its induced-permutation realization, and its quotient at is nonzero because its restriction contains its trivial source. Applied to a block , the quotient at is . Together with the maximal-subgroup characterization of defect from Question 1, this proves that its bimodule vertices are precisely for its defect groups . The integral conclusion follows by orbit-sum reduction and idempotent lifting.
Finally
Apply the just-proved Green correspondence with ambient group . Its unique vertex- summand of lies in : outside there is no -fixed group-basis point, as in Question 2. Since the indecomposable summands of are exactly its block ideals, this summand is a block with defect group . Conversely induction of has as its unique vertex- summand. The block bijection is the Brauer correspondence of Question 2, giving the claimed block form over either coefficient ring.
For the final special case put with a trivial-intersection Sylow subgroup. For , the intersection has order prime to . Indeed every -subgroup of it lies both in the normal Sylow subgroup of and in , whose intersection is trivial. Mackey decomposition therefore gives
where every other double-coset term is induced from a group of order prime to . By Maschke's theorem such modules are projective, and induction preserves projectivity, so is projective.
Every nonprojective -module has nonprojective restriction to : is prime to , so averaging makes the module a summand of the induction of its restriction. A projective restriction would therefore make the original module projective. Decompose into indecomposables. Each nonprojective summand contributes a nonprojective summand on restriction, whereas the displayed Mackey formula and Krull–Schmidt theorem have exactly one nonprojective summand, , with multiplicity one. There must be one, since is nonprojective. Hence
Here is an involution form of the double-coset criterion for a one-point extension. Embed in by fixing , choose , and put . The necessary and sufficient condition is the existence of an involution such that
Products in this part are compositions of maps, with the rightmost map applied first. The criterion is a finite test on permutations of the enlarged set; it does not presuppose that a larger group has already been found.
For sufficiency, put . Multiplying a double coset by an element of on either side leaves it unchanged. A product of two elements of reduces to . If , then ; otherwise the last condition puts it in . Hence is closed under multiplication. It contains the identity and is closed under inverses, since , so it is a group.
Every element sends to , whereas elements of fix . Thus . Moreover the orbit of contains and then all of , so is transitive and is the desired one-point extension of a permutation group. For the order check, : an element of the intersection fixes both and , and the reverse containment follows from . Consequently , as required.
For necessity, let be an extension. It is doubly transitive group action, of order , which is even. By Cauchy theorem for groups it contains a nontrivial involution, and a pair interchanged by this involution can be carried to by double transitivity. Conjugating gives an involution interchanging these two points. Their common point stabilizer is , so . Finally has just two orbits on the enlarged set, namely and , giving . More explicitly, for , choose with ; then fixes and belongs to . If , the element moves , so it belongs to , completing necessity.
The Hecke operators organize modular forms simultaneously by their transformation law and their Fourier coefficients. Work with , its space of weight- modular forms, and its cusp form subspace, with even . Odd weights give zero spaces. The normalization below makes the first coefficient of equal to the th coefficient of , which is the key link between operators and arithmetic.
For with positive determinant, the determinant-normalized slash operator for modular forms is
The automorphy factor identity proves . Positive scalar matrices act trivially. Let be the integral matrices of determinant . Left multiplication by reduces their first column, by Bezout identity, to with ; the determinant then gives . A row shear makes . These are unique determinant-n matrix representatives for Hecke operators, so define
Right multiplication by any element of permutes these left cosets. The slash operator for modular forms identity therefore proves that has the same modular transformation law as . Each summand is holomorphic on the upper half-plane. Its cusp behavior follows explicitly from the coefficient calculation below, so preserves both and .
Insert in the sum. The finite sum over is zero unless , in which case it is . Writing leaves the term with multiplier . Thus the Fourier coefficients of a composite-index Hecke operator are
For use . In particular the constant coefficient becomes , so cusp forms remain cusp forms, and
for a prime number . The absence of negative powers proves cusp holomorphy. Notice that no primality assumption is needed in the composite-index formula.
The Hecke multiplication relations can be derived directly, rather than assumed from the coset description. On Fourier series define auxiliary maps and . They need not separately preserve , but . With , the coefficient formula gives
Multiplying on the left by , the term in the sum contributes ; the terms with become . Together with the sum this is exactly . Hence the Hecke prime-power recurrence from q-shift operators is
For coprime , substituting the coefficient formula twice gives a sum over and with coefficient . The divisors correspond uniquely to a divisor , so . The prime-power recurrence, by induction on the smaller exponent, gives
Combining the coprime and prime-power formulas proves
In particular the Hecke operators commute, and the modular Hecke algebra is generated by the prime operators.
The analytic reason for simultaneous diagonalization is the Petersson inner product
which is positive definite on and convergent because of exponential cusp decay. Here is the adjoint argument. For a matrix , set . The left cosets in are represented by with . Unfolding this finite coset sum in the Petersson inner product gives
Under , hyperbolic area is unchanged and the determinant factors in the slash operator for modular forms give
The integration group becomes . Folding this finite cover back to identifies the adjoint with the correspondence for . For , the matrix is again integral with determinant ; scalar matrices act trivially, and adjugation permutes the double cosets making up . The real normalizing factor is unchanged. Thus this proves that Hecke operators are self-adjoint for the Petersson inner product:
The valence formula for the modular group makes a finite-dimensional vector space. Commuting self-adjoint operators on a finite-dimensional inner product space have a common orthogonal eigenbasis: diagonalize one operator, use commutativity to preserve each of its eigenspaces, and repeat within those spaces. Therefore has a basis of Hecke eigenforms, with real Hecke operator eigenvalues.
If is a common Hecke eigenform, say , its first Fourier coefficient cannot vanish: would imply for every . Normalize . Then the Hecke operator eigenvalue is precisely the Fourier coefficient . The Hecke multiplication relations become
Consequently the coefficients are multiplicative at coprime indices, and their local generating function satisfies
This gives the Euler product of a Hecke eigenform
in a half-plane of absolute convergence. The Fourier coefficient bound for a cusp form already supplies such a half-plane; Question 4 improves it to .
The L-function of a cusp form also has an analytic description independent of the Hecke eigenform condition. Termwise Mellin transform in an initial right half-plane gives
At infinity the cusp form decays exponentially. Modular inversion gives , so at zero it is . The integral therefore converges locally uniformly for every , continuing to an entire function. Changing to proves
For a normalized Hecke eigenform, the Euler product of a Hecke eigenform and this functional equation describe the same completed L-function of a cusp form.
There is also an integral arithmetic structure. One standard consequence of the level-one dimension formula and the valence formula for the modular group is the integral triangular basis of level-one modular forms: if with , choose respectively. Then
form a basis of , and the terms form a basis of . Their first nonzero terms are with coefficient one and all coefficients are integers. Successive elimination of coefficients of shows that these cusp basis elements generate exactly the lattice of rational cusp forms with integral Fourier coefficients. The composite-index coefficient formula preserves this lattice, so each has an integral matrix on it. Its characteristic polynomial is monic with integral coefficients. This proves that Hecke eigenvalues are algebraic integers; self-adjointness also makes every root of that characteristic polynomial real. The field generated by the eigenvalues is a finite totally real number field: a finite set of operators spans the finite-dimensional rational modular Hecke algebra, and every conjugate of each eigenvalue remains a root of its real-rooted characteristic polynomial.
Two basic examples connect the operator theory to familiar modular forms. The normalized Eisenstein series has coefficients proportional to . At a prime number its coefficient formula uses
where the second term is zero unless . This follows by writing with and summing a finite geometric series. It proves , and the Hecke multiplication relations give . Meanwhile implies , because . Thus the Ramanujan tau function is multiplicative and satisfies . For example, gives . This illustrates how Hecke operators turn analytic Fourier coefficients into a coherent arithmetic system.
Use the usual Krull–Schmidt theorem setting, in which indecomposable summands have local endomorphism rings; the paper's rings satisfy it for the subgroups involved. The relative projective module condition for means that is a direct summand of a module induced from , equivalently, is a summand of . A vertex of an indecomposable module is an inclusion-minimal such subgroup. A source of an indecomposable module at its module vertex is an indecomposable -summand of such that .
Existence of a module source follows by decomposing and using Krull–Schmidt theorem on the induced decomposition: the indecomposable summand must occur in the induction of one indecomposable summand . Such has module vertex as a -module, since relative projectivity of for a proper subgroup would make relatively projective for that subgroup.
In the paper's modular coefficient rings, an indecomposable module is a trivial source module when its module source is the rank-one trivial module of its module vertex. It is then a summand of , a permutation module. Conversely suppose is an indecomposable summand of a permutation module. Restriction to a module vertex is a sum of modules , one for each -orbit of the permutation basis. For a -group , each transitive permutation module is indecomposable: over it has simple head of a module over the local ring , and over a nontrivial splitting would give a nontrivial splitting after reduction. A module source must be one of these summands by Krull–Schmidt theorem. Its module vertex is , whereas is relatively -projective. Thus , and . Therefore trivial module source is equivalent to being an indecomposable permutation-module summand.
The rank-one formulation uses the paper's coefficient rings. If the earlier general coefficient-ring wording were applied to a disconnected ring, it would need qualification: for and , is an indecomposable summand of the permutation module , but is not the rank-one trivial module . One can instead allow indecomposable summands of the trivial coefficient module as module sources in that generality.
For the homomorphism request, take . Frobenius reciprocity and Mackey decomposition give
The summand for is generated by the sum of the cosets in the -orbit of . The identical orbit-sum construction over gives one copy of per double coset. These are free bases in both characteristics, since invariance means coefficients are constant on orbits, with no division by orbit size. Hence
The same argument applies to direct sums of coset permutation modules.
If is a trivial module source -module, choose a permutation lattice with . Its projection is an idempotent . The endomorphism reduction is surjective by the preceding calculation. Its kernel is , and the endomorphism algebra is complete over . By idempotent refinement theorem, lifts to an idempotent . The lattice is a permutation-module summand, hence a trivial module source lattice, and reduces to .
To prove uniqueness within the class of trivial module source lattices, let be two such lifts. They are summands of permutation lattices. Lift a modular isomorphism and its inverse between them by the same homomorphism-surjectivity argument, inserting the summand projections on either side. The lifted composites are identity modulo and therefore invertible over , by Nakayama lemma or the determinant criterion. The lifted maps are consequently inverse up to an invertible composite and give . Thus each trivial module source module has a unique trivial module source lift up to isomorphism. This is permutation homomorphisms lift through modular reduction; uniqueness is not claimed among arbitrary lattice lifts.
A fiber bundle with base , fiber and structure group acting on from the left consists of a projection and local trivializations . On overlaps they satisfy
The smooth transition functions are valued in . A principal bundle is the case with the left multiplication action on itself; its transition functions multiply the group coordinate from the left.
In each principal chart define . This defines a global right action because : coordinate changes commute with right multiplication. It is free, and acts transitively on each fiber. Thus the claimed right action follows from the left transition convention rather than being an additional choice.
If is a global section of a fiber bundle, define by . Freeness and transitivity give exactly one for every point in the fiber, so is bijective and equivariant. In a local trivialization where has group coordinate , the inverse group coordinate is , proving smoothness of the inverse. Hence is a principal-bundle trivialization. Conversely, the identity coordinate in a product trivialization gives . Therefore
This is the principal bundle trivialization by a global section criterion. It is special to principal bundles; a section alone need not trivialize an arbitrary fiber bundle.
For the quotient examples, assume the Lie subgroups are closed when smooth homogeneous-space statements are intended. The map is a principal bundle with structure group and right action ; is a homogeneous space for left multiplication by . Similarly, has free transitive left action on its fibers. With the usual principal right-action convention one writes . The quotient is a homogeneous space for right multiplication by . These quotients are groups only when the respective subgroups are normal. Nonclosed immersed Lie subgroups can produce non-Hausdorff quotients, so an arbitrary Lie subgroup does not automatically give a smooth Hausdorff base.
Left and right multiplication commute, so taking their orbit equivalence relations in either order gives the same double coset set
This equality does not assert that the double quotient is a manifold or that either stage is a principal bundle. The action can have stabilizers: they correspond to . If the induced action is free and proper, its quotient is a smooth principal-bundle quotient; without those hypotheses orbit dimensions can change. For example, with and both subgroups the rotations fixing the third axis, double cosets are parametrized by . Interior and endpoint stabilizers differ, so this is not a uniform free principal-bundle construction.
For a principal bundle and a left action on , the associated bundle is
with projection . A local principal section gives coordinates , and its changes give precisely the left action of the principal transition functions on . A linear action on a vector space gives an associated vector bundle.
For a metric of signature on an -manifold, an orthonormal frame at is an isometry . The orthonormal frame bundle has structure group , acting on the right by . Its associated bundle for the standard representation is the tangent bundle, since
is well defined: . Every tangent vector has exactly one such associated equivalence class, and local frame coordinates show that this is a vector-bundle isomorphism. The full frame bundle works similarly with .
Finally, choose a basis of the Lie algebra of a Lie group . Its left translates are a global frame, yielding the explicit tangent bundle trivialization
This proves parallelization of a Lie group by left translations and triviality of the full frame bundle. Choosing an inner product at the identity and translating it gives a left-invariant Riemannian metric; an orthonormal basis translates to a global orthonormal frame. The global section criterion therefore trivializes the corresponding orthonormal frame bundle as well. For any other positive-definite metric on , smoothly applying the Gram-Schmidt process to this global frame gives the same conclusion. Thus the tangent and frame bundles of every Lie group are trivial; the orthonormal statement is with respect to a chosen metric as specified above.
Here is the double-coset criterion for a one-point extension. Let , and suppose swaps and . Then is a one-point extension if and only if
For necessity, in an extension fixes both and , so normalizes it and lies in it. Since is transitive on , the extension has exactly two double cosets relative to : and . For , moves into and is in the latter double coset.
For sufficiency, the displayed conditions make closed under multiplication. Products with middle element in reduce using ; those with middle element outside remain in . A finite nonempty multiplication-closed set of permutations containing the identity is a group. It contains and , hence equals . Every element in moves , while fixes it, giving the required stabilizer subgroup. The group is transitive because is transitive on and moves the additional point.
False. Realize the symmetries of a square as a dihedral group of order eight, generated by and , with and . Take . Its double cosets are precisely
These are disjoint and exhaust the eight symmetries. There are three double cosets, and . This proves that double-coset counts need not divide group order. Specifying the order-eight realization avoids competing conventions for the notation of a dihedral group.
False. Use the same subgroups of . The double coset has two elements, while has four. Thus even a fixed pair of subgroups can give different double-coset sizes. Their disjoint union is all six elements of .
False. Let and . For , direct multiplication gives the double coset
It has four elements, and . This is a concrete example of double-coset sizes not dividing group order; Lagrange's theorem applies to subgroups, not to arbitrary double cosets.
Every lies in , since both subgroups contain the identity. If two double cosets intersect, choose
Then , so every element of lies in . Reversing the argument gives equality. Thus the double cosets partition the group.
Unlike single cosets, double cosets can have different cardinalities. For finite , decompose into left cosets of , or apply the orbit-stabilizer theorem to the action of on . Its stabiliser subgroup is , giving
This formula explains the counterexamples in the following parts.
For a finite group , subgroups , and a complex group representation of , the Mackey restriction formula is
Choose one representative of each double coset . The conjugate subgroup representation is a representation of on the same vector space, with . Restriction of a representation keeps the vector space and restricts the acting subgroup. induced representation is , and analogously for each subgroup of . The displayed isomorphism is an isomorphism of -representations. These definitions specify every summand and its subgroup.
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.
There is an index error in the displayed identity of the original PDF. With its definition of the signed Young permutation module, the tensor identity for induced representations gives
Both superscripts must be . In particular , rather than the printed sign twist of . For , , the printed left side has dimension , while the printed right side has dimension one. Thus that identity cannot hold as written.
The requested character inner product between and nevertheless has a well-defined answer. Let be the row Young subgroup of a tableau of shape , and let be its column subgroup, conjugate to . By Frobenius reciprocity and the Mackey restriction formula, the inner product is a sum over of
These double cosets are encoded by nonnegative integer matrices with row sums and column sums , recording intersection sizes of row and column blocks. The intersection subgroup is a product of . Its sign representation is trivial exactly when every . Each zero-one matrix contributes one, and every other matrix contributes zero.
There is exactly one zero-one matrix with these margins. Its first row has length , equal to the number of nonzero column sums, so that row must consist entirely of ones. Delete it, subtract one from every column margin and discard zero columns. The remaining margins are those of and its conjugate partition; induction forces the rest. The unique matrix is precisely for . Therefore
This calculation uses the actual two modules requested in the PDF and does not depend on its erroneous displayed isomorphism.