This is the degree-one convention for an almost commutative algebra: the exhaustive filtration is generated by a finite-dimensional first step containing , the degree-zero part is , and its associated graded algebra is commutative. The first step is a finite-dimensional Lie algebra under commutators. Its inclusion into extends by the universal property to a surjection from its universal enveloping algebra. The element of the first step is retained as a central Lie generator and its image is the associative identity; quotienting the first step by before taking the bracket can lose scalar commutators. This convention is stronger than merely requiring a finitely generated commutative associated graded algebra for an arbitrary weighted filtration.
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Free graded Lie algebra 2026-10-14
For a positively graded vector space , the free graded Lie algebra receives a linear map from and extends every graded linear map uniquely to a Lie homomorphism. Over , it is the Lie subalgebra generated by inside the tensor algebra , using . Its universal enveloping algebra is : both have the same universal property for maps from into associative algebras. The primitives of the tensor Hopf algebra with primitive generators are exactly .
Generalized Weyl algebra 2026-10-14
For a ring , an automorphism and central , adjoin with , , and . This construction includes Weyl algebras and rank-one universal enveloping algebras.
For a graded Lie algebra over characteristic zero, the associated graded algebra of its universal enveloping algebra under the word-length filtration is its graded symmetric algebra. Ordered homogeneous monomials form a basis, with exponent at most one on each odd Lie basis element. The defining graded commutation relations reorder every word, and the Jacobi identity resolves the triple-reordering ambiguities. In particular the primitive elements of a Hopf algebra of are precisely : in its associated graded algebra, a primitive polynomial of symmetric length greater than one would have a nonzero mixed term under the diagonal, which is impossible in characteristic zero.
Hermitian quantum generator convention Created 2026-10-06 Updated 2026-10-14
For a unitary derived representation , its generators are anti-Hermitian. Define Hermitian observables ; then their ordinary operator commutator is . Thus real Lie algebra structure constants and Hermitian-operator commutation relations differ by an . Products in a universal enveloping algebra require one conversion factor for every generator. In particular, the abstract bilinear Pauli-Lubanski element has representation image minus the pseudovector formed from the Hermitian physical generators.
Milnor–Moore theorem 2026-10-14
For simply connected , rational Hurewicz homomorphism identifies with the primitive elements of a Hopf algebra of and induces an isomorphism of graded Hopf algebras. The bracket on homotopy is the Samelson product. The underlying algebra theorem says that a connected graded cocommutative Hopf algebra over characteristic zero is the universal enveloping algebra of its primitive Lie algebra. These statements let a free tensor algebra of loop-space homology detect a free graded Lie algebra of homotopy.
Choose a basis of the Lie algebra and filter its universal enveloping algebra by word length: and is spanned by products of at most basis elements. The relations replace a degree-two commutator by degree one, so the degree-one symbols commute.
The Poincaré-Birkhoff-Witt theorem says the ordered monomials are a basis. Its relevant proof can be seen by reordering an inverted neighboring pair using the displayed relation. Reordering terminates because same-length terms have fewer inversions and bracket terms have smaller word length. Disjoint swaps commute; the only overlapping three-letter reorderings differ by . The Jacobi identity therefore makes the reduced ordered expression independent of the reordering path. Ordered monomials have no remaining relations and form the basis. Their degree- symbols give
For generators of the finitely generated module , put . This is a good filtration, and is finite over the three-variable polynomial ring. Define the dimension of a filtered module as the Krull dimension of its associated graded module, equivalently the degree of the eventual cumulative polynomial , or the Gelfand–Kirillov dimension of a module. Two good filtrations have bounded shifts, so the growth degree is independent of the generators. Since
its polynomial degree is at most three. Therefore every nonzero finitely generated -module has dimension at most . The zero module may be assigned the usual separate empty-support convention. This bound also follows immediately from its support of a module inside affine three-space.
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.
Let . Its quotient cell structure has one cell in each of dimensions . In particular is five-connected. The relative cohomology sequence, or its cellular cochain complex, gives
The subscripts denote degrees. Under the quotient map back to , the three positive classes pull back to . All positive products vanish, since their degree is at least twelve. Thus the cohomology ring of a collapsed projective subspace in this case is the square-zero algebra on these three classes.
Now compute its Sullivan minimal model , using cohomological grading and the convention that even generators generate a polynomial ring and odd generators an exterior algebra. Five-connectivity gives for . Since a minimal differential is decomposable, it cannot have a nonzero value below degree twelve. Matching cohomology through degree ten therefore forces
with no other generators in degrees at most ten. The first products must then be killed by generators
These follow by killing respectively the unwanted degree-twelve, degree-fourteen, and two degree-sixteen classes. Subsequent generators kill and the resulting syzygies. For example is closed of degree nineteen, so it requires a further generator of degree eighteen. Thus the full minimal model is not just the algebra on the first seven generators.
There is nevertheless a simple map from the full model to : send to the three displayed classes and every other generator to zero. It is a chain map, since every generator differential is a sum of products of positive-degree elements, and all positive products in vanish. It induces an isomorphism in cohomology: the entire cohomology of is concentrated in degrees , and its indicated basis maps to the indicated basis of . This proves formality of a topological space and identifies the full minimal model as a minimal resolution of , rather than only matching the initial part of its cohomology.
An explicit description of that full resolution is useful. Take the free graded Lie algebra
Its Chevalley–Eilenberg cochain algebra has one generator of degree for every homogeneous Lie basis word , and its quadratic differential is dual to the bracket, with the usual graded signs. Rescaling the bracket-word duals gives exactly the generators and differentials listed above. Positive Lie degrees make this algebra Sullivan minimal. Its cohomology is : the universal enveloping algebra is , and the augmentation module has the exact free resolution
Exactness is immediate because every nonempty tensor word has a unique last letter. Applying gives just the unit and the three dual classes in total degrees ; products of positive classes land in an absent Ext degree two and are zero. Chevalley–Eilenberg cochains of a graded Lie algebra compute this Ext, so this also verifies the full model's cohomology.
The wedge sum has the same connectivity, cohomology ring, and initial closed minimal generators. The same full-model-to- argument applies to , so its minimal model is also , by uniqueness of Sullivan minimal models of quasi-isomorphic simply connected rational cochain algebras. The Sullivan minimal-model classification identifies isomorphic minimal models with the same rational homotopy type. Consequently
The explicit infinite minimal resolution above is shared by both spaces.
Use the degree-one convention implicit in this enveloping-algebra assertion: a degree-one almost commutative algebra has , a finite-dimensional containing which generates , and commutative associated graded ring. Taking the leading symbol of a commutator gives
in particular . Thus , equipped with , is a finite-dimensional Lie algebra. Bilinearity and antisymmetry are immediate, and expanding the three nested commutators proves the Jacobi identity.
Its inclusion into the associative algebra is a Lie algebra homomorphism. The universal enveloping algebra is modulo the relations . Sending the tensor generators to their elements of kills these relations and gives an algebra homomorphism . It is surjective because generates . Therefore
The vector is retained as a central Lie algebra generator and maps to the associative identity; its corresponding relation in the kernel is that generator minus . One should not first replace by , since commutators of generators can be nonzero scalars.
Terminology is important here. Merely requiring a commutative finitely generated associated graded ring for an arbitrary weighted filtration is a broader definition of almost commutative algebra; it does not supply the finite-dimensional bracket-closed first step used in this argument. The degree-one assumptions make the requested enveloping presentation precise. The Noetherianity in part (b) also follows directly under the broader finite-generation convention.
An almost commutative algebra over has an exhaustive nonnegative increasing multiplicative ascending filtration
for which the associated graded ring
is a commutative finitely generated complex algebra. This includes the customary degree filtration with , finitely many degree-one generators, and commutators lowering degree. The finite-generation clause is part of the convention used here and is necessary for the conclusion.
A finitely generated commutative complex algebra is a quotient of a polynomial ring . Repeated application of the central-variable case of the Hilbert basis theorem makes that polynomial ring Noetherian; quotients preserve the ascending chain condition by lifting ideal chains. Thus is Noetherian.
We prove ascending filtered-graded transfer of Noetherianity directly. Give a left ideal the induced ascending filtration . Its associated graded module embeds into as a homogeneous ideal, denoted . Choose finitely many homogeneous generators of this ideal, of degrees , and lifts . Homogeneous generators may be chosen by taking homogeneous components of any finite generating set.
For , its degree- symbol can be expressed as
with terms of negative coefficient degree omitted. Lift each coefficient to . Then
Induction on , ending at , expresses in the left ideal generated by the . Hence every left ideal is finitely generated. Applying the same argument to right ideals, or to the opposite ring, proves
This degree-lowering proof terminates in finitely many steps and requires no completeness assumption on the filtered ring. Without finite generation of the graded algebra, a counterexample would be the commutative polynomial ring in infinitely many variables, whose ideals do not stabilize.
For the universal enveloping algebra , use the degree ascending filtration inherited from the tensor algebra of the finite-dimensional Lie algebra . For , the defining relation is , whereas the product has filtration degree at most . Thus the degree-one symbols commute in . Those symbols generate the graded algebra, so it is a quotient of
This already proves the required almost-commutative property. The Poincaré-Birkhoff-Witt theorem gives the stronger identification , but injectivity of this map is not needed for the chain-condition argument. Therefore
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.
First consider finite-dimensional Lie algebra representations. The operators representing an abelian Lie algebra commute. They have a common eigenvector: take an eigenspace for the first operator of a basis of the algebra, observe that every remaining operator preserves it, and repeat inside this nonzero space. The resulting line is an invariant subspace, so an irreducible representation must be one-dimensional. Its action has the form for a linear functional . Conversely, every such functional defines a Lie algebra representation, since both the Lie brackets in the algebra and the commutators of its scalar operators vanish. Distinct functionals give nonisomorphic representations. Thus the irreducibles are precisely the characters .
Indecomposable does not imply irreducible. For the one-dimensional abelian Lie algebra , let act on by the Nilpotent Jordan block
The line spanned by the first coordinate vector is an invariant subspace, so the module is reducible. If it were a direct sum of two nonzero submodules, both would have dimension one; nilpotence would force to act as zero on both, contrary to . Thus it is an indecomposable representation.
For a finite-dimensional module , put and define its generalized weight spaces intrinsically by
To obtain the decomposition, choose a basis of , split into generalized eigenspaces of , and successively split each piece by . All the pieces are submodules because the acting operators commute. On one resulting piece, has a unique eigenvalue . The commuting operators can be simultaneously upper triangularized by repeating the common-eigenvector argument on quotients. Hence on this piece every is strictly upper triangular. Any linear combination is also strictly upper triangular, and its th power vanishes. Extending linearly therefore identifies the piece with . Different tuples give disjoint pieces; if a component has a different tuple from , at least one is invertible there. Consequently
with only finitely many nonzero summands. Since the definition uses every rather than a chosen basis, this generalized-weight decomposition for a nilpotent Lie algebra is canonical. Its summands need not be irreducible, as the Jordan block example already shows.
Let be the given invariant bilinear form on a Lie algebra. Choose a basis and its -dual basis , so . The Casimir element is
The tensor is the inverse tensor of , so it is independent of the chosen basis. Multiplication in the universal enveloping algebra therefore makes independent of that choice as well.
For , write . Invariance means , whence . Therefore
by interchanging in the second sum. Since generates its universal enveloping algebra, is central. This argument does not require adding a symmetry assumption to the given bilinear form.
For the sl2 Lie algebra, take
The cyclic identity for the trace gives . The form is nondegenerate, since , , and all the other pairings except are zero. The dual of is , so
By the classification of finite-dimensional sl2 representations, an irreducible of dimension has a highest-weight vector with and , where . Since , one obtains
Centrality and the Schur lemma then give the answer on the entire representation:
This Casimir eigenvalue for sl2 depends on normalization. Choosing the Killing form instead, , scales the dual basis and the Casimir element by , giving .
Choose a base of a root system and its positive roots, so that the triangular decomposition of a Lie algebra is . A primitive element of a Lie algebra representation of weight is a nonzero vector such that
Equivalently it is a highest-weight vector. Being primitive depends on the chosen positive system; no integrality condition is part of this definition.
Construct the Verma module for an arbitrary . The subalgebra has a one-dimensional module on which acts by and acts by zero. This is a representation because . Set
where denotes the universal enveloping algebra. The Poincaré-Birkhoff-Witt theorem, applied with negative-root vectors first, then Cartan vectors and positive-root vectors, gives
as vector spaces. In particular is nonzero, generates , and is primitive of weight .
The same ordered monomials show that is a direct sum of weight spaces, with weights of the form
and that its weight- space is exactly . Each vector has only finitely many weight components. If a submodule contains a vector with nonzero weight- component, choose that separates from the finitely many other weights of that vector. Polynomial interpolation in the action of extracts a nonzero multiple of . Such a submodule is all of , because generates it. Consequently every proper submodule has zero component in weight .
Let be the sum of all proper submodules. Every finite sum still has zero weight- component, so is proper; it contains every proper submodule and is therefore the unique maximal proper submodule. Its quotient
is irreducible, and the nonzero image of is primitive of weight . This proves existence for every and gives the irreducible quotient of a Verma module. It also proves uniqueness up to isomorphism among irreducible modules generated by a primitive vector of that weight: the defining relations induce a surjection from , whose proper kernel must be .
These modules are not generally finite-dimensional. For example, in an root subalgebra, a primitive vector with satisfies
If its irreducible highest-weight module is finite-dimensional, the weight-lowering sequence eventually stops. For the first with and , the identity forces . In general a finite-dimensional highest-weight module therefore requires nonnegative integral values on all simple coroots; arbitrary in the request must allow infinite-dimensional representations. This is consistent with the finite-dimensional qualification made in Question 2.
For simple coroots forming a basis of , the fundamental weights are the dual basis :
For the special linear Lie algebra , take the diagonal trace-zero Cartan subalgebra and positive roots corresponding to upper triangular matrix units. Write . The simple roots are , , and the simple coroots are
The fundamental weights of sl3 are therefore
Checking these on gives the two coordinate vectors and . In the Euclidean trace-zero plane they can also be written
The Fundamental representations of sl3 make these weights concrete: has primitive vector of weight , and has primitive vector of weight . Every finite-dimensional irreducible highest weight is with nonnegative integers .
Use the metric in the question and fix the Levi-Civita symbol convention . A consistent choice of rotation Lie algebra generators is
Substituting the indices into the printed Poincare algebra gives
The other cyclic brackets follow the same way. The negative spatial metric and antisymmetry of both enter this sign.
The printed brackets are real Lie algebra brackets, without the factor used for ordinary commutators of Hermitian quantum observables. We use those brackets for the algebraic verifications. For physical eigenvalues below, angular momentum is Hermitian, its spin projection is the real number , and . In that quantum convention the ordinary operator commutators are times the displayed brackets. This distinction prevents identifying a real spin projection with an anti-Hermitian matrix eigenvalue.
In the universal enveloping algebra, translations commute. The Pauli-Lubanski pseudovector therefore satisfies
For fixed , the product of momenta is symmetric in while the epsilon coefficient is antisymmetric in them. There is no need to commute the Lorentz generator through the momenta.
Using the commutator derivation identity and the mixed bracket,
The two terms become equal after swapping , and the last expression vanishes by antisymmetry in . In the Hermitian observable convention, the calculation has one overall extra and still vanishes. Thus preserves each momentum eigenspace.
For the specified epsilon orientation, two useful component identities are
The order displayed matters: the momentum operator is on the right, so it can act first on the momentum eigenstate. At rest, , and on a spin state with these give
These are massive rest-frame Pauli-Lubanski eigenvalues. The raised component would be ; confusing with reverses the answer.
Helicity is the projection of spin angular momentum, or equivalently the rotation generator acting internally, along the momentum direction:
For the momentum with , the helicity operator is . Hence a helicity- state has
The result uses only the two longitudinal components and does not need a separate assumption about the transverse little-group generators. These massless longitudinal Pauli-Lubanski eigenvalues agree with for ordinary finite-helicity representations.
Finally, at rest the contraction is . For the chosen null momentum it is , whose two eigenvalues cancel. Thus both results obey . Reversing the epsilon orientation reverses all eigenvalues together; it leaves both identities and both consistency checks intact. For a literal anti-Hermitian derived representation of the printed real algebra, write for the Hermitian observable. Since is bilinear in generators, its abstract enveloping-algebra image is . Thus the corresponding formal-image eigenvalues, if that convention is intended, are
Here has eigenvalue , while and themselves remain real physical labels. This is the same result after the Hermitian quantum generator convention is applied to both factors, not an inconsistent choice of spin sign. Both the Hermitian-observable and literal anti-Hermitian interpretations are consequently specified.
Schur's lemma says that a nonzero intertwiner between irreducible representations is an isomorphism; over , every endomorphism of a finite-dimensional irreducible representation is scalar. To prove the Schur lemma, let be a intertwining operator between irreducible representations. Its kernel and image of a linear map are invariant. If , irreducibility forces and . This proves the first assertion over any field. In particular the endomorphisms of an irreducible representation form a division ring.
When is finite-dimensional over an algebraically closed field, an endomorphism has an eigenvalue . The endomorphism has nonzero kernel. By the first assertion it must be zero, so . Consequently, for complex finite-dimensional irreducible representations, the space of intertwining operators has dimension zero for nonisomorphic representations and dimension one for isomorphic representations.
Every finite-dimensional representation of a complex semisimple Lie algebra is completely reducible. We prove the Weyl complete reducibility theorem using the allowed Casimir operator facts, without assuming a splitting in advance. For dual bases with respect to the Killing form, the Casimir element
is central in the universal enveloping algebra. Hence its Casimir operator commutes with the action on every Lie algebra representation and is compatible with subrepresentations, quotient representations, and intertwining operators. On the trivial Lie algebra representation it acts by zero. On every nontrivial finite-dimensional Irreducible Lie algebra representation it acts by a nonzero scalar.
For clarity, the last fact can be expressed by the Casimir eigenvalue formula: on an irreducible with dominant integral weight , the scalar is , with the inner product induced by the Killing form and the half-sum of positive roots. On the real span of the weights this inner product is positive definite, and the scalar is positive for . For a semisimple Lie algebra with several simple factors the scalars add, so a nontrivial representation still gives a nonzero scalar. These are properties of the Casimir operator being used here.
First establish Casimir splitting of a trivial quotient. Suppose
is a short exact sequence of finite-dimensional Lie algebra representations, with trivial quotient. The generalized eigenspaces of are invariant, so
Each with maps to zero under : applying a sufficiently large power of and using gives . Thus .
Take a composition series of a module of . The Casimir operator is nilpotent on , so its scalar on every irreducible composition factor is zero. The stated Casimir operator property makes every such factor trivial. In a basis adapted to the composition series of a module, the image of on therefore consists of strictly upper triangular matrices, so that image is solvable. The allowed fact that a semisimple Lie algebra acts trivially on every one-dimensional representation implies that is a perfect Lie algebra: otherwise a nonzero linear functional on would define a nontrivial one-dimensional Lie algebra representation. Thus , and its image is consequently a perfect Lie algebra too. A perfect Lie algebra that is also a solvable Lie algebra is zero, since its derived series of a Lie algebra is constant until it vanishes. Hence acts trivially on . Choose with . The map is an invariant section, proving the split short exact sequence assertion.
Now let be any nonzero subrepresentation. On the Hom representation the action is
Consider the invariant subspace
Restriction produces a short exact sequence
Surjectivity follows by extending to a linear map on . The quotient is trivial, because commutes with the action on . The preceding Casimir splitting of a trivial quotient yields an invariant with . Thus
and is invariant. The zero subrepresentation also has a complement. Repeatedly splitting off an irreducible subrepresentation now gives a direct sum of irreducibles, proving the Weyl complete reducibility theorem.
A derivation of a Lie algebra is a linear map satisfying the Leibniz rule
The space is a vector subspace of . Equip it with the commutator . Expanding the Leibniz rule twice gives
Subtracting proves that is again a derivation of a Lie algebra. Antisymmetry and the Jacobi identity hold for the commutator in every associative endomorphism algebra, so this defines the derivation Lie algebra.
The Jacobi identity says that is a derivation of a Lie algebra. Moreover, for ,
so
This makes an ideal of a Lie algebra in .
Finally suppose is semisimple. Let act on by . The Weyl complete reducibility theorem supplies an invariant complement to . For , invariance gives , while the ideal identity above gives . Their intersection is zero, so for every . The center of a Lie algebra of a semisimple Lie algebra is zero, hence for every , and . Therefore
Every derivation of a Lie algebra is inner, and the element giving it is unique because the center of a Lie algebra vanishes.