The Baker--Campbell--Hausdorff formula converges integrally on a powerful Lie lattice. A degree- Lie term has bracket divisibility ; the standard integral coefficient bound loses at most powers of . The remaining valuation tends to infinity. Associativity follows from the formal exponential identity, the identity is zero, the inverse is , and . The resulting pro-p group is a uniform pro-p group, with power subgroups .
On the set underlying a uniform pro-p group, define scalar multiplication by , and define addition and the Lie bracket by
Roots are the unique roots in the appropriate power layers. The limits give a powerful Lie lattice. In a suitable complete normed group algebra, the p-adic logarithm identifies these operations with ordinary addition and the associative-algebra commutator.
Every uniform pro-p group embeds continuously in for some finite . Apply the Ado theorem to and choose a deep power lattice whose representing matrices lie in , or at . The matrix exponential and logarithm give a faithful representation of the corresponding open normal power subgroup. Induce that representation to the whole group using its finitely many cosets. An element outside the open subgroup permutes the coset blocks nontrivially; an element inside it is detected by the original representation. Thus the induced representation is faithful. All block matrices preserve a finite free -module, giving the integral embedding.
For an odd prime , the matrix logarithm and matrix exponential are inverse maps between and . They imply that the th-power map carries bijectively onto . Direct multiplication gives , so the group is a powerful pro-p group. The quotient is the additive matrix space over , with constant index . The matrices topologically generate, by successive approximation through these quotients. The lower p-series is exactly , so the group is a uniform pro-p group and a torsion-free group. At the first congruence subgroup contains and is not uniform.
A uniform pro-p group is a finitely generated powerful pro-p group whose lower p-series , has constant successive indices. For odd , the powerful pro-p group condition means , with closed generated powers understood. For it means . For finitely generated powerful pro-p groups, uniformity is equivalent to being a torsion-free group.
It is convenient to use general matrix size , then put . Let . The required kernel is , the inverse limit of its finite p-group quotients. For odd , the convergent matrix logarithm and matrix exponential series
are inverse maps between and . The valuation bounds for ensure convergence and integrality. They give and hence a bijective power map : the unique root of is .
Direct matrix multiplication gives , so and it is a powerful pro-p group. Moreover
The elements topologically generate: their th powers give all matrix basis directions in , since . Successive correction of each matrix entry, followed by completeness, approximates every element by words in these generators.
Its lower p-series is exactly and the indices are constant; thus the group is a uniform pro-p group. Alternatively, the logarithm excludes nontrivial p-power torsion. Setting gives a uniform pro-p group kernel of dimension and generator number , with indices . This is the odd-prime principal p-adic congruence subgroup is uniform result. The odd-prime condition matters: is nontrivial order-two torsion in .
In the uniform pro-p group , the -th power of is exactly , and its unique -th root in the appropriate layer is division by . The intrinsic addition is therefore
The linear term is exact; every non-linear term tends to zero by the convergence estimates above. The intrinsic Lie bracket is
since the leading term is and the terms of degree at least three vanish after rescaling. Finally the intrinsic scalar operation sends to . All underlying sets are identical, and all three operations agree. Thus
Put and , where powers mean closed generated subgroups. The finite-quotient arguments of Question 3 pass to a powerful pro-p group: in particular is powerfully embedded, the power map is onto , and
For the root assertion, apply the finite result to every finite quotient and use the finite intersection property on the closed sets of possible roots in the compact group. Each is finitely generated by the appropriate powers of a finite generating tuple, and is finite and elementary abelian. Thus the are open. They form an identity-neighbourhood basis: in any finite continuous quotient their images form a terminating lower p-series, so some is contained in the kernel. In particular . Collection also gives
One can see the extra index directly by induction from : collect for . Its leading factor advances one layer, and the remaining iterated commutators, with their binomial coefficients, lie at least as deep. Products and limits preserve the inclusion. This is the usual strongly central property of the lower p-series.
A uniform pro-p group is a finitely generated powerful pro-p group for which all the indices equal . The preliminary congruence gives surjective linear maps
If is uniform, these maps are bijective. If , write and choose the unique layer with . Bijectivity of and the power congruence imply , so . Thus the power map is injective. A finite-order element of a pro-p group has -power order; repeated injectivity of the power map excludes every nonidentity such element. Hence a uniform group is a torsion-free group.
Conversely, suppose some has a nonzero kernel. Choose with . At step , if the current satisfies , surjectivity of supplies with
Set . The power congruence gives . Since the corrections tend to in the complete profinite group, the converge to , with and . In particular . A torsion-free group cannot have such an element, so every is injective and all layer indices are equal. This proves the root correction criterion for uniformity and
For a uniform group the power maps are continuous bijections , hence homeomorphisms. Their inverses define the unique roots used below. Comparison at the first differing layer also proves the power congruences in a uniform pro-p group:
The intrinsic Lie algebra of a uniform pro-p group has the same underlying set as , zero equal to the group identity, and operations
Here is the limit of integral powers approaching . The first root is taken in and the second in ; the commutator actually lies in . The following faithful algebra realization verifies convergence and the Lie algebra axioms, rather than assuming them as part of the definition.
Choose a minimal tuple of topological generators. The layer isomorphisms show that the images of are bases of . The ordered-coordinate argument of Question 3 therefore gives a continuous bijection
Existence follows by successive digits and compactness; uniqueness follows by the first digit at which the coordinates differ, because its images are linearly independent in the corresponding power layer. Thus this map is a homeomorphism.
Here are details of the norm needed on the group algebra. In put . Its elements have unique ordered expansions with . To verify this description, identify the ordered coordinates of with . Elements of the completed group algebra are integral measures on this space; their values on the binomial polynomials are precisely the coefficients . The finite-difference identity pairs the ordered monomial with this binomial polynomial as . The Mahler expansion of a continuous function therefore proves both existence and uniqueness of the measure with the specified coefficients. This also proves that the ordinary rational group algebra embeds in these expansions.
Choose and set
This defines the weighted group algebra of a uniform pro-p group. Its multiplication is submultiplicative in the valuation convention, . Indeed, has valuation ; collection of ordered coordinates gives the same lower bound for when . Interchanging two adjacent in a product introduces a correction coming from , of valuation at least . Iterating the interchange rule never lowers the total weight; the corrections have strictly increasing weight, so infinite collection converges. The same argument with -th powers shows
The equality follows from the first nonzero coordinate digit: its leading terms are , at least one with unit , and cannot cancel in the ordered expansion. Completing the rational group algebra in this norm produces a complete normed algebra in which embeds faithfully and with its original topology.
Since , the series
converge on the relevant balls in and are inverse there. Their convergence follows from and ; formal one-variable identities prove that they are inverse. Put and . The Baker--Campbell--Hausdorff formula in now gives
because every term of degree at least two tends to zero after this rescaling. Similarly expansion of gives
The leading term is the indicated associative-algebra commutator and all terms of degree at least three tend to zero. These expressions are the logarithms of the unique roots in the intrinsic formulas. The image is compact and hence closed in , so both limits belong to , and the inverse logarithm takes the limits back to . Also . Consequently identifies the intrinsic operations with addition, scalar multiplication and commutation in . The Jacobi identity follows by expanding the associative products; thus is indeed a Lie algebra over .
The commutator roots in the intrinsic formula belong to , so their limit gives . Iterating the power congruence gives . Taking the unique roots shows that intrinsic addition modulo is the original group product modulo . Consequently is the original elementary abelian quotient , and the images of the form a basis. Successively removing digits expresses every element uniquely as an additive sum : existence uses completeness, while a nonzero relation would have a first nonzero digit contradicting the basis in . Hence is a free module of rank over the p-adic integers and is a powerful Lie lattice.
Conversely a powerful Lie algebra over p-adic integers, for odd , is a finite free -module with a bilinear alternating Lie bracket satisfying the Jacobi identity and . Define
For completeness, integrality and convergence can be verified without guessing which individual denominators are units. In set . Then , so its integral universal enveloping algebra has an ordered basis by the Poincaré-Birkhoff-Witt theorem. Its coefficientwise -adic norm is submultiplicative, and consists of elements of valuation at least one. The homogeneous degree- terms in have coefficients of valuation at least : expand the logarithm, use on each nonconstant exponential factor, and on a product of such factors. Therefore evaluating degree on gives valuation at least
which tends to infinity and is at least two when . Each homogeneous term is a rational Lie polynomial by the formal Baker--Campbell--Hausdorff formula. The ordered enveloping-algebra basis shows that its intersection with is exactly , so the estimate places the sum in , with the non-linear part in .
Associativity follows from the identity in the completed universal enveloping algebra. Its identity is , its inverse is , and , since the bracket of with itself is zero. The same coefficient estimate for the group commutator puts it in . Conjugation in the BCH group is ; each term preserves , because each bracket adds a factor of and . Thus the submodules are normal subgroups for , their intersection is zero, and their finite quotients have -power order. Thus is a powerful pro-p group, with
A module basis topologically generates this group: it generates the quotient , and successive power digits lift that generation through all . The BCH construction therefore gives a uniform pro-p group.
The proof of the linearity of a uniform pro-p group has three distinct steps: pass to a finite-dimensional Lie algebra, integrate a faithful representation on a sufficiently small open subgroup, and extend it to the entire group. Working first on a small subgroup is essential because a faithful Lie algebra representation need not send the original integral lattice into the convergence domain of the matrix exponential.
Let be a uniform pro-p group and let be its intrinsic powerful Lie lattice. Then
is a finite-dimensional Lie algebra over a field of characteristic zero. The Ado theorem, the classical Lie-theoretic ingredient in this proof, supplies a faithful finite-dimensional Lie algebra representation
One must use a faithful representation rather than just the Adjoint representation, which annihilates the center of a Lie algebra.
Choose a p-adic lattice . Since is finitely generated as a module, the entries of the representing matrices of a module basis have bounded denominators. Hence for sufficiently large ,
For odd , the matrix exponential and p-adic logarithm converge and are inverse between and . Put ; under the uniform pro-p group and powerful Lie lattice correspondence it is the BCH group on . Define
Here denotes the inverse of the intrinsic logarithm identification, not an assumed matrix representation of . The Lie algebra homomorphism respects the convergent Baker--Campbell--Hausdorff formula, so
Thus is a continuous group homomorphism. If , taking the matrix logarithm gives , whence . Therefore is faithful and all its matrices preserve . This proves linearity of the open normal subgroup .
To finish, use the extension of a faithful representation from an open normal subgroup. Choose representatives of the finite left cosets , where . On the finite free module , define the action of by writing uniquely
and mapping the -th block to the -th block by . If and , then ; this proves the representation identity because . Each block matrix is invertible over , and the map is continuous because the finite coset permutation is locally constant and the remaining matrix entries are obtained continuously from .
If , its permutation of moves the identity coset, so its block representation is not the identity. If and its block representation is the identity, the block corresponding to is , and faithfulness of gives . Thus this induced representation is faithful. Choosing a basis of proves
The continuous injection is a topological embedding, since is compact and the target is Hausdorff. The trivial group is immediate. For uniform groups at , the same proof uses the usual stronger powerfulness condition and the convergence ball instead; the preceding questions concern odd .
Conversely, if all equal , the same Frattini-quotient identity gives for every . This is exactly the index definition of a uniform pro-p group. Thus (ii)(i), completing the equivalence of the first two conditions.
For a pro-p group, the lower p-series is the descending sequence of closed characteristic subgroups
The bar means closure of the subgroup generated by the displayed powers and group commutators. Throughout this question is odd. For a finitely generated powerful pro-p group, group commutator collection gives , each is powerful, and . All these subgroups are open. A uniform pro-p group is such a group with all subgroup indices equal to . We use the standard powerful-group torsion criterion: a finitely generated powerful pro-p group is uniform exactly when it is a torsion-free group. For a uniform group of generator number , the indices are , and is a homeomorphism from onto .
We record explicitly the collection facts used for the operations below. With , one has
The second statement is the power-congruence property: the th-power map is an isomorphism on adjacent uniform layers, and collection gives for . Thus the first nonzero layer of a difference moves down exactly one step under a th power. Iterating gives the asserted equivalence and also justifies taking roots of congruences. These facts follow from powerful-group group commutator collection, using divisibility by of and the successive-layer power isomorphisms; they are the uniform-group structure results being used here.
The transported addition on a uniform pro-p group is
The product is in and has a unique th root in . For the comparison at define . The numbered proofs below establish associativity, approximate commutativity and compatibility of these operations.
The intrinsic Lie algebra of a uniform pro-p group has underlying set , zero equal to the group identity, additive inverse , and operations
Here the group commutator is . For , is the limit of for integers ; the pro- topology makes it well defined. The addition sequence is Cauchy by the compatibility proved below. The group commutator estimate puts in , so its displayed root exists and lies in . Collection of group commutators shows that successive bracket approximants differ in layers tending to the identity, giving the other limit. The group commutator identities give additivity of the limiting bracket, and the Hall-Witt identity gives its Jacobi identity. Approximate commutativity makes limiting addition commutative. The resulting lattice is a free module over of rank , and .
A powerful Lie algebra over p-adic integers, in the convention relevant here, is a Lie algebra whose underlying module is finite free over and whose bracket satisfies . For the condition is instead . For odd , define multiplication on its underlying set by the convergent Baker--Campbell--Hausdorff formula
An iterated bracket of degree lies in . The BCH coefficient bound loses at most powers of , so all higher-degree terms are integral, and their valuations tend to infinity. This explains both convergence and why multiplying a lattice with small bracket stays inside the lattice. Formal associativity of BCH passes to the convergent series, the identity is , the inverse is , and every group power satisfies . The quotients by are finite p-groups. Hence the resulting compact group is a finitely generated torsion-free group and a pro-p group, and its group commutator lies in . Thus is a uniform pro-p group, with and successive index .
The standard uniform-group/Lie-lattice correspondence identifies these constructions as mutually inverse: and . To see why the inverse limits recover the lattice operations, the addition approximant for a BCH group is : its linear term is and every higher term tends to zero. Similarly its group commutator approximant has limiting term . In the other direction, a local logarithm in the complete normed group algebra identifies the intrinsic operations with algebra addition and commutator and identifies group multiplication with BCH; the uniform power maps extend the identification from a sufficiently small power subgroup to all of . Continuous group homomorphisms respect powers, unique roots and limits, while Lie algebra homomorphisms respect every BCH term, so the equivalence also preserves morphisms.
The objective is a continuous faithful representation of a uniform pro-p group in some . The proof proceeds from the intrinsic Lie lattice to a small matrix group, then extends the resulting representation to all of . This last step matters: a representation defined only on an open subgroup does not yet establish linearity of the original group.
Let be the Lie algebra of a uniform pro-p group and put . The uniform-group/Lie-lattice correspondence identifies the group law on with BCH. The substantial finite-dimensional Lie-theoretic input is the Ado theorem: every finite-dimensional Lie algebra over a characteristic-zero field admits a faithful finite-dimensional representation. Apply it to obtain
An Adjoint representation would not suffice here, since it kills the centre; Ado supplies injectivity even in central directions.
Choose a p-adic lattice spanning . Since has finitely many lattice generators, their representing matrices have bounded denominators. There is therefore an integer such that
On this matrix lattice the series and converge and are inverse. For example , so the valuations of the exponential terms tend to infinity with this choice of ; the logarithm terms do as well. They take values in and in respectively. The formal identity holds for the convergent series.
Under the correspondence, has Lie lattice and is an open characteristic subgroup. Define
where denotes the identification of with . A Lie homomorphism preserves BCH, so the exponential identity proves . If , the matrix logarithm gives ; faithfulness of gives . Thus is a continuous faithful integral representation of .
To extend it, take the module
Values on a transversal of determine , so is a free module over of rank . These functions are continuous, since on each open coset they are given by the continuous representation . Define . The equivariance condition is preserved, and . In a transversal basis each is a permutation of blocks followed by matrices from , so it belongs to and depends continuously on .
Faithfulness can be checked directly. If , right multiplication moves the coset to a different coset, so moves a function supported on one block and cannot be the identity. If and , evaluation at gives for every , whereas equivariance gives . Since is arbitrary, , and hence . Therefore
Compactness of makes this continuous injection a homeomorphism onto its closed image. This proves the linearity of a uniform pro-p group for the full group, including its centre, and explains why taking a sufficiently small power lattice permits matrix integration before finite-index induction restores the whole group.
The correspondence concerns uniform pro-p groups and powerful Lie lattices, with their natural morphisms. Put for odd and for . A powerful pro-p group is a pro-p group whose closed commutator subgroup lies in its closed -power subgroup. It is uniform when it is topologically finitely generated and all successive indices in its lower p-series are equal. Equivalently, a finitely generated powerful pro-p group is uniform precisely when it is a torsion-free group. A powerful Lie algebra over p-adic integers means a Lie algebra over that is free of finite rank as a module and satisfies
Here a Lie algebra over a ring is a module with an alternating bilinear Lie bracket satisfying the Jacobi identity. Finite freeness is an essential part of the lattice convention. The zero-bracket module satisfies the bracket inclusion but has torsion, and its additive group is not uniform. Thus allowing arbitrary torsion modules would make the categorical assertion false.
The basic structural facts behind the construction can be seen from the power layers. Write with . Collection for a powerful pro-p group gives
For odd , the power lifting is exactly the successive-correction argument of Question 3, followed by compactness; at the stronger fourth-power commutator condition makes the corresponding collection corrections work. The maps between successive layers are surjective linear maps. Uniformity makes their finite dimensions equal, so these maps are isomorphisms. Comparing the first layer in which two elements differ now shows that the power map is injective, while the power-set formula makes it surjective. Thus all the roots used below exist uniquely in the indicated layer. If lift a basis of , the images of form a basis of . Successively choosing their coefficients modulo gives the unique ordered expression
Existence follows by lifting one layer at a time and taking a limit; uniqueness follows by comparing the first nonzero coefficient layer. In particular and these layers form a neighbourhood basis. These are the power-layer and coordinate facts needed in the proof, rather than an assumption that an arbitrary pro-p group has unique roots.
On the underlying set of , set the additive zero to , the additive negative of to , and define
The p-adic integers act through limits of integer powers in the closed cyclic subgroup generated by . In the second formula the product belongs to ; in the third the group commutator belongs to . The symbols and denote the unique group roots, not unrestricted division in a group. We next justify convergence and the Lie algebra laws together.
A useful concrete tool is a complete normed group algebra containing . In its completed group algebra, put . Ordered-coordinate uniqueness gives unique expansions with . To see why, first work modulo and : the ordered products of the with exponents below form the regular basis, and the change to the corresponding products of is triangular with diagonal entries one. Take inverse limits and then lift the coefficient digits successively in powers of . Define the weight
It is a genuine separated, submultiplicative weight. Indeed reordering produces a group-commutator correction in ; the binomial expansion of a th power gives that correction weight at least , so collection never decreases total weight. Also . Inverting and completing therefore gives a Banach algebra over . For , ordered coordinates show
with value infinity at . Thus the induced topology on is exactly its original topology. This construction supplies the ambient algebra without presupposing the uniform pro-p group and powerful Lie lattice correspondence. The weighted construction, including the case , is described in Equivariant D-modules on rigid analytic spaces, Section 6.5.
Since , the p-adic logarithm and p-adic exponential converge on the relevant balls in :
The estimates and show that term weights tend to infinity. Formal substitution is legitimate there and proves that the two maps are inverse. They preserve the leading weight. In particular embeds the compact set homeomorphically into , and .
Put and . Expanding the convergent Baker--Campbell--Hausdorff formula in gives
The first expansion has linear part and all other terms have degree at least two in . The second has leading term and all remaining terms have degree at least three. After division by the displayed powers of , the extra factor of forces those errors to zero. The normalized expressions are logarithms of the unique roots already specified. Since is compact and closed in , both limits belong to . Scalar multiplication also remains in by continuity of powers. Consequently is a module over , closed under the associative-algebra Lie bracket . Bilinearity, alternation and the Jacobi identity follow by expanding products in the associative algebra . Transporting these operations back gives exactly above.
The commutator-layer inclusion places every normalized bracket root in . Since and this set is compact, passage to the limit proves . Addition modulo is the original multiplication modulo : collection shows , as the nonlinear errors lie at least one layer deeper. Thus has dimension , with basis . Given , write its residue as and repeat on . This iterative digit lifting converges because the remainders stay in the bounded compact set . It gives with . A nontrivial relation among the could be divided by the smallest power of among its coefficients, contradicting their independence modulo . Hence is free of rank , proving that it is a powerful Lie lattice.
Conversely, let be a powerful Lie lattice. In , define
The formal Baker--Campbell--Hausdorff formula and its coefficient estimate are the algebraic ingredients used here. More precisely, the degree- component can be expressed as an integral Lie polynomial divided by a number of -adic valuation at most . One way to obtain this estimate is to bound the associative coefficients of and use an integral ordered basis of the free Lie algebra. The denominator bound , where is the base- digit sum, is at most . A precise primary reference for that denominator estimate is Smallest common denominators for the homogeneous components of the Baker-Campbell-Hausdorff series. A length- Lie bracket in lies in . Thus the degree- term belongs to
These exponents are nonnegative and tend to infinity; for they are at least one. This proves integral convergence, continuity and . Associativity follows from the formal identity in the completed universal enveloping algebra. Substitution of three elements is justified by the same valuation estimates, so the two associative expressions agree. The identity is , the inverse is , and because every nonlinear term involving only vanishes.
For powerfulness, formal conjugation gives
The difference lies in : its th term has valuation at least for . The group commutator is therefore . Its linear term is . Every nonlinear Lie term contains , since it vanishes when , and the extra divisibility makes all those terms lie in too. Hence . The ideals are open normal subgroups for , and their finite quotients have order . The group is consequently a pro-p group. Its power sets are exactly , its lower-series indices are constantly , and a basis of topologically generates it by the same successive digit lifting. The BCH group is uniform.
To check the inverse constructions, powers in the Baker--Campbell--Hausdorff formula group are ordinary multiples in . Therefore
and the similarly normalized group commutator tends to . The limit constructions recover the original Lie algebra exactly. In the other direction, the ambient Banach algebra construction gives , so the recovered operation is the original multiplication of .
Finally a continuous group homomorphism between uniform pro-p groups preserves integer powers and powers with exponents in the p-adic integers, preserves the unique roots in the power layers, and commutes with their limits. It therefore becomes a linear Lie algebra homomorphism. Conversely a linear Lie algebra homomorphism between finite free modules is continuous and preserves every term of the convergent Baker--Campbell--Hausdorff formula, hence is a continuous group homomorphism for . The constructions preserve identity maps and composition, and the inverse identifications are natural. They are mutually inverse functors, giving the stated category correspondence with the finite-free lattice convention.
For a uniform pro-p group with , the map transports congruences by
Commutator collection gives for , and the power map is an isomorphism . Thus a nontrivial first difference moves down exactly one layer when taking a th power. Iterating gives the equivalence; completeness supplies unique roots when the congruence is read in reverse.
A Lie algebra over the p-adic integers whose underlying module is free of finite rank and whose Lie bracket satisfies , where for odd and for . Finite freeness is part of this convention: merely requiring a small Lie bracket on a torsion module would not correspond to uniform pro-p groups.
Powerful pro-p group 2026-10-14
A pro-p group whose closed commutator subgroup lies in its closed power subgroup , with for odd and for . This is the profinite analogue of a powerful p-group. Finitely generated torsion-free examples are exactly the uniform pro-p groups. The additive group of a finite product of p-adic integers is an abelian example.
For odd and a finitely generated powerful pro-p group, put . The displayed group homomorphisms are surjective. If one has a nonzero kernel, choose with . Successive corrections , with , cancel its -th power one layer at a time, using . Compactness and the separated power filtration give a nonidentity limit of order . Thus a torsion-free group has constant layer indices and is a uniform pro-p group. Conversely constant indices make every displayed map injective; comparison at the first differing power layer proves that is injective, so there is no nontrivial torsion.