A New Proof of the Existence of Free Lie Algebras and an Application

The existence of free Lie algebras is usually derived as a consequence of the Poincar´e-Birkho ﬀ -Witt theorem. Moreover, in order to prove that (cid:3) given a set X and a ﬁeld (cid:0) of characteristic zero (cid:4) the Lie algebra L (cid:3) (cid:0) (cid:2) X (cid:3) (cid:4) of the Lie polynomials in the letters of X (cid:3) over the ﬁeld (cid:0) (cid:4) is a free Lie algebra generated by X , all available proofs use the embedding of a Lie algebra (cid:0) into its enveloping algebra U (cid:3) (cid:0) (cid:4) . The aim of this paper is to give a much simpler proof of the latter fact without the aid of the cited embedding nor of the Poincar´e-Birkho ﬀ -Witt theorem. As an application of our result and of a theorem due to Cartier (cid:3) 1956 (cid:4) , we show the relationships existing between the theorem of Poincar´e-Birkho ﬀ -Witt, the theorem of Campbell-Baker-Hausdor ﬀ , and the existence of free Lie algebras.


Introduction
We begin with the main definition we will be concerned with in this paper. In the sequel, Definition 1.1. Let X be any nonempty set. We say that L is a free Lie algebra generated by X if L is a Lie algebra, and there exists a map φ : X → L satisfying the following property. For every Lie algebra and for every map f : X → , there exists exactly one Lie algebra morphism f φ such that the diagram below commutes When X ⊂ L set-theoretically and the above property is satisfied with the inclusion map ι : X → L replacing φ, L will be called a free Lie algebra over X.
It is easy to see that a free Lie algebra generated by X-if it exists-is unique up to Lie algebra isomorphism. The existence of a free Lie algebra generated by a set can be proved in a standard way see 1, Chapitre II, Section 2, n.1 and 2, Section 0.2 . As for the existence of a free Lie algebra over a set, it is natural to expect that given a field Ã of characteristic zero the Lie Ã -algebra of the Lie polynomials in the letters of X is a free Lie algebra over X. To prove this fact, however, more profound results are required, as we will explain below.
In the sequel, if V is a vector space, we denote by T V its tensor algebra and by L V the smallest Lie-subalgebra of T V containing V . The aim of this paper is to prove the following result. Theorem 1.2. Let Ã be a field of characteristic zero, and let Ã X be the free vector space generated by X, then L Ã X is a free Lie algebra over X.
Classically, the above theorem is derived from the theorem of Poincaré, Birkhoff, and Witt henceforth referred to as PBW , which we here recall for the reading convenience and to fix some notation.

Theorem of Poincaré-Birkhoff-Witt
Let Ã be a field of characteristic zero, and let be a Lie algebra. We denote by U the universal enveloping algebra of and by 1 the unit element of U . Let π denote the natural projection π : T → U , and let us set μ : π| . Suppose that is endowed with an indexed linear basis {x i } i∈I , where I is totally ordered by the relation , then the following elements form a linear basis for U : 1, μ x i 1 · · · μ x i n , where n ∈ AE, i 1 , . . . , i n ∈ I, i 1 · · · i n .

1.2
As a by-product of this theorem, we have the following crucial result.
The above corollary is the essential tool one needs in order to prove Theorem 1.2. To the best of our knowledge, all the books using free Lie algebras prove Theorem 1.2 by making use of Theorem PBW or, precisely, of Corollary 1.3 ; see Bourbaki 1, Chapitre II, Section 3, n.1, Théorème 1 where it employed 3, Chapitre I, Section 2, n.7, Corollaire 3 du Théorème 1 which is the PBW Theorem ; see Reutenauer 2, Theorem 0.5 where the injectivity of → U is used ; see also Hochschild 4, Chapter X, Section 2 , Humphreys 5, Chapter V, Section 17.5 , Jacobson 6, Chapter V, Section 4 , and Varadarajan 7, Section 3.2 .
For the sake of completeness, let us briefly recall the argument which uses PBW. Proof. The universal property of T V allows us to prove the existence of exactly one morphism of associative algebras F such that the following diagram commutes: It is easily seen that F t ∈ μ for every t ∈ L V , so that we can compose the restriction of F to L V with μ −1 : μ → the function μ −1 is well posed on μ thanks to Corollary 1.3 . The map satisfies all the requirements in the statement of the lemma.
Let us now prove Theorem 1.2 with the aid of Lemma 1.4 above. Let X be any set and let , f be as in Definition 1.1. Let us denote by φ the inclusion map X → L Ã X . We apply Lemma 1.4 with V Ã X and F obtained by prolonging the function f by linearity on V , then the Lie algebra morphism F : L Ã X → is easily seen to satisfy the requirements of f φ in Definition 1.1, and Theorem 1.2 is proved.
The aim of this paper is to provide a new proof of Theorem 1.2, independently of PBW and of Corollary 1.3. This will be done in Sections 2 and 3.
The remainder of the paper Section 4 provides a motivation for the first part. The occasion to search for a proof of Theorem 1.2 which is alternative to the usual one arose when-in our studies in monograph 8 -we came across a nonstandard demonstration of Theorem PBW due to Cartier 9 . Cartier's proof uses the Theorem of Campbell, Baker, and Hausdorff CBH, shortly in order to prove PBW. In its turn, CBH is usually proved by means of Theorem PBW see, e.g., Bourbaki 1, Chapitre II, Section 3, n.1, Corollaire 2 , Hochschild 4, Proposition 2.1 , Jacobson 6, Theorem 9, Chapter V , and Serre 10, 11, Theorems 4.2, 7.1 . So Cartier shows that, beside the usual argument PBW ⇒ CBH, 1.5 surprisingly, the reverse path can be followed too.
In order to make this reverse path "CBH ⇒ PBW" fully consistent, it is necessary to provide a proof of CBH which is independent of PBW. Seemingly, apart from Hausdorff's original argument 12 , an algebraic proof of CBH independent of PBW was not available at the time of Cartier's paper 9 , dated 1956. Twelve years later, Eichler 13 gave another proof, using only free Lie algebras, and then seven years after Eichler, Djoković 14 provided another one, using formal power series computations. More recently, Reutenauer 2, Section 3.4 has proved CBH with a rigorous algebraic formalization of the early ideas by Pascal, Baker, Campbell, and Hausdorff. See 8, Chapters 1, 4 for more details on all these topics. Cartier provides this proof in 9 , making use of free Lie algebras generated by a finite set. As long as the existence of free Lie algebras is again a consequence of PBW, clearly it cannot be exploited to prove Theorem PBW itself. Hence, in 9 a proof of the existence of free Lie algebras generated by finite sets is given, independently of PBW, and relying only on the ideas contained in the classical proof of the theorem of Dynkin, Specht, and Wever. By making use of these ideas, we here provide a proof, with no prerequisites, of the existence of free Lie algebras over arbitrary sets, thus generalizing the result in 9 . We hope that a new proof, which is alternative to all those presented in books, is welcome, especially since it makes no use of such a deep result as the Theorem of Poincaré, Birkhoff, and Witt. As an application, we are able to highlight the full interdependence of PBW and CBH and the existence of free Lie algebras see Section 4 , which-to the best of our knowledge-has never been pointed out in the specialized literature so far see Theorem 4.1 and Corollary 4.3 .

The Free Lie Algebra Generated by a Set
In the present short section, included for the sake of completeness and to fix the notation used throughout, we recall an argument, which dates back to Bourbaki 1, Chapitre II, Section 2, n.1 see also Reutenauer 2, Section 0.2 proving directly the existence of free Lie algebras generated by a set.
For n ∈ AE, n ≥ 1, consider the set M n X also denoted by M n , for short of all roughly speaking the noncommutative, nonassociative words of length n on the elements of X. The M n s can be defined inductively by means of disjoint unions denoted by of Cartesian products in the following way: Let M X : n≥1 M n X . We can define a noncommutative, nonassociative binary operation on M X as follows. For any w, w ∈ M X , say, w ∈ M n and w ∈ M n , we denote by w · w the unique element of M n n corresponding to w, w in the canonical injections M n × M n ⊂ M n n ⊂ M X . This binary operation endows M X with the structure of a magma, called the free magma generated by X. Let us now set Lib X : Ã M X , the free vector space generated by the free magma M X . The free vector space generated by a set M is here thought of as the Ã -vector space of the functions from M to Ã vanishing outside a finite set; equivalently, it will be treated as the set of formal finite linear combinations of elements of M, where M is a basis for Ã M . The canonical map M X → Lib X sending w ∈ M X to the characteristic function of {w} in M X will be simply denoted by set inclusion. The operation on M X extends by linearity to an operation on Lib X turning it into a nonassociative algebra, called the free (nonassociative) algebra generated by X. We have the following result, whose proof is standard and hence omitted. Given an not necessarily associative algebra M, * , we say that S ⊆ M is a twosided magma ideal in M if S is a vector subspace of M such that s * m and m * s belong to S, for every s ∈ S and every m ∈ M. Moreover, if H ⊆ M is any set, the smallest two-sided magma ideal in M containing H will be said to be the magma ideal generated by H in M.
Let us now consider the algebra Lib X and We henceforth denote by the magma ideal generated by A in Lib X . We next consider the quotient vector space Lie X : Lib X / and the natural projection π : Lib X → Lie X . Then the map is well posed, and it endows Lie X with a Ã -algebra structure, which turns out to be a Lie algebra over Ã see the very definition of A .

Proposition 2.2.
Let X be any set and, with the above notation, let us set ϕ : π| X : X → Lie X then 1 Lie X , together with the map ϕ, is a free Lie algebra generated by X (according to Definition 1.1); 2 the set {ϕ x } x∈X is independent in Lie X , whence ϕ is injective; 3 the set ϕ X Lie-generates Lie X , that is, the smallest Lie subalgebra of Lie X containing ϕ X , coincides with Lie X .
The proof of this proposition is derived by collecting together various results appearing in 1, Chapitre II, Section 2 , with the additional care of transposing them to a nonassociative setting see, e.g., 8, Theorem 2.54 for all the details .

The Isomorphism Lie X
L Ã X From now on, we turn to prove Theorem 1.2 without using neither Theorem PBW nor Corollary 1.3. The arguments are more delicate than those in the preceding section.
We fix throughout a field Ã of characteristic zero. We denote by L Ã X the smallest Lie subalgebra of T Ã X the tensor algebra of the vector space Ã X containing X. Let ϕ be as in Proposition 2.2. Being Lie X a free Lie algebra generated by X, there exists a unique Lie algebra morphism 3.1 Our main task is to show that Φ is an isomorphism, without using PBW theorem. This will immediately prove that L Ã X is a free Lie algebra over X, according to Definition 1.1. We will do this by means of some auxiliary functions.

ISRN Algebra
Lemma 3.1. With the above notation, one has the grading Lie X n≥1 B n , where B 1 span ϕ X , and, for any n ≥ 2, B n B 1 , B n−1 span ϕ x , y : x ∈ X, y ∈ B n−1 .

3.2
Proof. It is easy to prove the grading Lib X n Lib n X , where Lib n X is the span of M n X . On the other hand, a simple argument shows that is also the magma ideal generated by the elements with w, w , w ∈ M X . As a consequence, we have an analogous grading n n , with n ⊆ Lib n X , for every n ∈ AE. This gives Lie X n C n , where C n Lib n X / is spanned by the n-degree commutators of the elements of ϕ X bracketing is taken in arbitrary order . In its turn, we obviously have C n B n , where B n is the span of the "nested" brackets ϕ x 1 · · · ϕ x n−1 , ϕ x n · · · , for x 1 , . . . , x n ∈ X. 3.4 Finally, it is a simple proof to check that B n , B m ⊆ B n m for every n, m.
Thanks to Lemma 3.1, the following auxiliary map is well posed: δ : Lie X −→ Lie X , δ n b n : n nb n b n ∈ B n , ∀n ∈ AE .

3.5
In the remainder of the section, for any vector space V , we denote by End V the set of the endomorphisms of V . By the universal properties of the free vector space Ã X and of tensor algebras, there exists a unique morphism of unital associative algebras θ : T Ã X → End Lie X , such that θ x ad ϕ x , for every x ∈ X.
The diagram below gives an idea of the setting we are working in We are now ready for the following result see also Cartier 9, Lemma 1, page 242 , where finite Xs are considered ; part c of the lemma is the core of a result due to Dynkin 15 . In the following statement, we denote by T Ã X the ideal of T Ã X whose elements have vanishing zero-degree component. Lemma 3.2. With all the above notation, one has the following: a δ is a derivation of the Lie algebra Lie X and δ • ϕ ≡ ϕ on X, b g xy θ x g y , for every x ∈ T Ã X , y ∈ T Ã X , Proof. a Take elements t, t ∈ Lie X n≥1 B n see Lemma 3.1 , t n t n , t n t n , with t n , t n ∈ B n for every n ≥ 1, and t n , t n are definitively equal to 0, then we have

3.7
Moreover, from the definition of the B n s in Lemma 3.1, we have ϕ X ⊂ B 1 , so δ ϕ x ϕ x , for every x ∈ X. 3.8 b An inductive argument: if x k ∈ Ã T 0 V , b is trivially true, g k y kg y since g is linear and θ k g y kId Lie X g y kg y .

3.9
Thus, we are left to prove b when both x, y belong to T Ã X ; moreover, by linearity, we can assume without loss of generality that x v 1 ⊗ · · · ⊗ v k and y w 1 ⊗ · · · ⊗ w h with h, k ≥ 1, and the vs and ws are elements of X, θ v 1 ⊗ · · · ⊗ v k g w 1 ⊗ · · · ⊗ w h θ x g y .
3.10 8 ISRN Algebra c Let ξ ∈ Lie X, then c follows if we show that θ Φ ξ and ad ξ coincide note that they are both endomorphisms of Lie X . In its turn, this is equivalent to the identity of θ • Φ with the map ad: Lie X −→ End Lie X , ξ −→ ad ξ .

3.11
Now observe that both ad and θ • Φ are Lie algebra morphisms indeed, Φ is a Lie algebra morphism by construction, and θ is a Lie algebra morphism since it is a unital associative algebra morphism . Hence, the equality of ad and θ • Φ follows if we prove that they are equal on a system of Lie generators for Lie X , namely, on ϕ X recall Proposition 2.2-3.8 , for every x ∈ X, we indeed have

3.13
In the third and fourth equalities, we used b and c , respectively. Since g • Φ and δ are derivations of Lie X coinciding on ϕ X , d follows.

Theorem 3.3. Let Ã be field of characteristic zero.
If Φ is as in 3.1 , Φ is an isomorphism of Lie algebras.
Proof. From the very definition of δ and the fact that Ã has characteristic zero, it follows that δ is injective. From the identity g • Φ ≡ δ see d in Lemma 3.2 and the injectivity of δ, we immediately infer the injectivity of Φ. Since Φ is clearly surjective indeed, Lie X and L Ã X are Lie generated by ϕ X and X, respectively , the theorem is proved.
In order to explicitly show the relationship of the arguments we employed to prove Theorem 1.2 with the so-called Theorem of Dynkin, Specht, and Wever, we seize the opportunity to show that the latter is implicitly contained in Theorem 3.3 and Lemma 3. Corollary 3.4 Dynkin, Specht, and Wever . Let Ã be a field of characteristic zero. Consider the linear map P : T Ã X → L Ã X such that 3.14 for any x 1 , . . . , x k ∈ X. Then P is a projection, that is, P is surjective and it is the identity on Consequently, one has the following characterization of Lie elements:

3.15
Proof. The well-posedness and surjectivity of P are obvious. To prove that P is the identity on In the second equality, we used d of Lemma 3.2; in the third, we used the definition of δ and the fact that

The Relationship between the Theorems of PBW and of CBH
The deep intertwinement between PBW and CBH and the existence of free Lie algebras can be visualized in the following chain of equivalent statements. Then these results can be proved each by the aid of the other in the following circular sequence: Remark 4.2. Notice that statement c was proved in Section 3 above, without any prerequisite nor the aid of any of the other statements in Theorem 4.1. In particular, the isomorphism of Lie X the free Lie algebra generated by X with L Ã X the Lie algebra of the Lie polynomials in the letters of X can be proved independently of b and f , as we announced.
Proof. a ⇒ b : this is obvious by the definition μ x i π x i , b ⇒ c : this is the usual approach to the existence of free Lie algebras over a set recalled in the Introduction, c ⇒ d : this is obvious, d ⇒ e : the derivation of the Campbell-Baker-Hausdorff theorem from the existence of free Lie algebras over finite sets appears in Eichler's proof 13 , e ⇒ f : the proof of PBW from CBH with the joint use of free Lie algebras over finite sets is contained in Cartier's paper 9 , f ⇒ a : this is obvious.
As by-products of the previous theorem, we highlight the following corollaries, containing some probably unexpected facts. c The existence of free Lie algebras over finite sets is sufficient for the existence of all free Lie algebras over arbitrary sets.
d The existence of free Lie algebras proves the Poincaré-Birkhoff-Witt theorem (not only the reverse fact is true).