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Universal central extension of the Lie algebra of exact divergence-free vector fields

  • Bas Janssens ORCID logo EMAIL logo , Leonid Ryvkin ORCID logo and Cornelia Vizman
Published/Copyright: August 23, 2025

Abstract

We construct the universal central extension of the Lie algebra of exact divergence-free vector fields, proving a conjecture by Claude Roger from 1995. The proof relies on the analysis of a Leibniz algebra that underlies these vector fields. As an application, we construct the universal central extension of the (infinite-dimensional) Lie group of exact divergence-free diffeomorphisms of a compact 3-dimensional manifold.

Award Identifier / Grant number: INSMI PEPS JCJC 2024

Award Identifier / Grant number: EC 2023-2024

Award Identifier / Grant number: Higher Lie theory

Award Identifier / Grant number: PN-III-P4-ID-PCE-2020-2888

Award Identifier / Grant number: 639.032.734

Funding statement: Leonid Ryvkin acknowledges the support of the INSMI PEPS JCJC 2024, the Accueil EC 2023-2024 of the Conseil Académique de l’UCBL, and the DFG-project Higher Lie theory. Cornelia Vizman was supported by the Romanian Ministry of Education and Research, CNCS-UEFISCDI: project number PN-III-P4-ID-PCE-2020-2888 within PNCDI III. Bas Janssens was supported by the NWO grant 639.032.734 “Cohomology and representation theory of infinite-dimensional Lie groups”.

A A multivector field description of the de Rham complex

It will be convenient to identify α Ω n k ( M ) with the multivector field A Γ ( k T M ) using the volume form 𝜇. If α = ι A μ , we write α = A and A = α . Our sign conventions for contraction of multivector fields into a form are fixed by ι A B μ = ι B ι A μ . With this identification, the de Rham differential 𝑑 on Ω ( M ) and the Leibniz bracket on Ω n 2 ( M ) give rise to a differential δ ( A ) : = d ( A ) on Γ ( T M ) and a Leibniz bracket [ A , B ] : = [ A , B ] on Γ ( 2 T M ) .

Proposition A.1

The differential δ : Γ ( k T M ) Γ ( k 1 T M ) is given by

δ ( X 1 X k ) = 1 i < j k ( 1 ) k + i + j [ X i , X j ] X 1 X ̂ i X ̂ j X k + i = 1 k ( 1 ) k + i div ( X i ) X 1 X ̂ i X k .

Proof

The case k = 1 is the definition of divergence. The case 𝑘 follows from k 1 using

d ι X k ( ι X 1 X k 1 μ ) = L X k ι X 1 X k 1 μ ι X k d ( ι X 1 X k 1 μ )

and L X k ι X 1 X k 1 μ = div ( X k ) ι X 1 X k 1 μ j = 1 k 1 ι X 1 [ X j , X k ] X k 1 μ .

Corollary A.2

If α = ι X 1 X 2 μ , then X α = δ ( X 1 X 2 ) is given by

(A.1) X α = div ( X 2 ) X 1 div ( X 1 ) X 2 [ X 1 , X 2 ] .

Similarly, the Leibniz bracket on Γ ( 2 T M ) takes the following form.

Proposition A.3

The Leibniz bracket on Γ ( 2 T M ) is given by

[ X 1 X 2 , Y 1 Y 2 ] = [ δ ( X 1 X 2 ) , Y 1 ] Y 2 + Y 1 [ δ ( X 1 X 2 ) , Y 2 ]

or, equivalently, by

[ X 1 X 2 , Y 1 Y 2 ] = [ [ X 1 , X 2 ] , Y 1 ] Y 2 Y 1 [ [ X 1 , X 2 ] , Y 2 ] div ( X 1 ) [ X 2 , Y 1 ] Y 2 div ( X 1 ) Y 1 [ X 2 , Y 2 ] + ( L Y 1 div ( X 1 ) ) X 2 Y 2 + ( L Y 2 div ( X 1 ) ) Y 1 X 2 + div ( X 2 ) [ X 1 , Y 1 ] Y 2 + div ( X 2 ) Y 1 [ X 1 , Y 2 ] ( L Y 1 div ( X 2 ) ) X 1 Y 2 ( L Y 2 div ( X 2 ) ) Y 1 X 1 .

Proof

If α = ( X 1 X 2 ) and β = ( Y 1 Y 2 ) , then [ α , β ] = L X α β = L X α ι Y 2 ι Y 1 μ . Using L X α ι Y j = ι [ X α , Y j ] + ι Y j L X α for j { 1 , 2 } and L X α μ = 0 , we find

[ α , β ] = ι [ X α , Y 1 ] Y 2 + Y 1 [ X α , Y 2 ] μ .

Substituting (A.1) then yields the required result. ∎

In particular, if α = ι X 1 X 2 μ and β = ι Y 1 Y 2 μ , then [ α , β ] is obtained by inserting [ X 1 X 2 , Y 1 Y 2 ] into 𝜇.

B A compactly supported Poincaré Lemma with parameters

In the proof of Lemma 3.7, we needed a version of the compactly supported Poincaré Lemma with additional parameters. While the existence of such a Poincaré Lemma is intuitively clear, we could not find any reference with a compactly supported version, so we provide a proof here for the sake of completeness. We supply here an elementary geometric proof for a cube; an alternative approach would be to construct a parameterised version of the support-preserving Poincaré Lemma of [3] (cf. also [26]).

Let M , N be manifolds. We consider X = M × N with the foliation F = T M × 0 N . The foliated longitudinal forms Ω , 0 ( X ) = Γ ( X , Λ F ) are exactly the complex of differential forms along 𝑀, and their differential is the de Rham differential d M in 𝑀 direction, with 𝑁 being treated as a parameter. We denote its cohomology by H , 0 ( X ) = H , 0 ( M × N ) . Alternatively, we could see 𝐹 as a Lie algebroid (with the inclusion as the anchor) and the above cohomology is just the Chevalley–Eilenberg cohomology of this Lie algebroid. When 𝑀 admits a finite good open cover, the Künneth theorem for Lie algebroids [21, Theorem 6.6] implies H , 0 ( M × N ) = H dR ( M ) C ( N ) . In the context of foliations, this statement goes back at least to [7] (cf. also [2]). This allows us to prove the following.

Lemma B.1

Let us consider a precompact cube U × V R k × R n for k 2 and n 1 . Given a form α Ω k , 0 ( U × V ) such that

  • supp ( α ) U × V is compact,

  • U α = 0 as an element of C ( V ) ,

there exists a compactly supported form δ Ω k 1 , 0 ( U × V ) with d M δ = α .

Proof

First, we consider a slightly smaller cube U ′′ × V with supp ( α ) U ′′ × V such that U ′′ U U and V V are relatively compact sets. At the same time, we see R k as S k N , where 𝑁 is the north pole of the 𝑘-sphere.

  • The form 𝛼 extends by zero to a form α ̃ Ω k , 0 ( S k × V ) . The class of α ̃ is trivial since S k α ̃ = U α = 0 . (Here we implicitly use H , 0 ( S k × V ) = C ( V ) as follows from the above Künneth theorem.) Let β Ω k 1 , 0 ( S k × V ) be a primitive of α ̃ .

  • Let β ̃ = β | S k U ′′ ̄ × V . We have d M β = α ̃ | S k U ′′ ̄ × V = 0 . Since

    H k 1 , 0 ( S k U ′′ ̄ × V ) = H k 1 ( S k U ′′ ̄ ) C ( V ) = 0 ,

    the form β ̃ has a d M -potential γ Ω k 2 , 0 ( S k U ′′ ̄ × V ) .

  • Let ρ 1 C c ( S k U ′′ ̄ ) have compact support and be constantly 1 on S k U . Similarly, let ρ 2 C c ( V ) have compact support and be constantly 1 on a neighbourhood of V . We set δ = ρ 2 ( β d M ( ρ 1 γ ) ) .

By construction, d M δ = ρ 2 d ( β d M ( ρ 1 γ ) ) = ρ 2 α ̃ = α ̃ , so we only have to understand why 𝛿 is compactly supported in U × V . The term ( β d M ( ρ 1 γ ) ) is supported in U × V (since we have ( d M ρ 1 γ ) | S k U ̄ = β | S k U ̄ ). Consequently, 𝛿 is supported in U × V which is precompact in U × V . ∎

C A Poincaré Lemma for differential operators

In this section, we will establish a Poincaré type lemma for differential operators, which we need for the proof of Theorem 4.7. First, we briefly recall Peetre’s Theorem for support-decreasing linear operators. For partial derivatives, we will use the notation

σ f : = ( x 1 ) σ 1 ( x n ) σ n f

with σ = ( σ 1 , , σ n ) N n as usual.

Theorem C.1

Theorem C.1 (Peetre [29])

Let E , F be vector bundles over 𝑀 and let

P : Γ c ( E ) Γ c ( F )

be a support-decreasing linear map. Then there exists a discrete set Λ M such that P | M Λ is continuous. Moreover, the restriction of 𝑃 to M Λ is a differential operator of locally finite order: for any p M Λ , there exist a chart ( U , x ) and frame { e i } of E U and finitely many nonzero distributions T i σ Γ c ( F | U ) such that

P ( s ) = i = 1 rank ( E ) σ N n ( σ s i ) T i σ

for all s = s i e i Γ c ( E | U ) .

The original result [29] was stated for open subsets of R n and for trivial line bundles, but the above version easily reduces to this because the statement is local. In detail, we have the following proof.

Proof

Let 𝒱 be a locally finite cover of 𝑀 such that 𝐸 and 𝐹 trivialise over every V V . Let e i and f j be the corresponding C ( V ) -bases of Γ ( E | V ) and Γ ( F | V ) , and write s = i s i e i and t = j t j e j for sections of E | V and F | V , respectively. Then

P i j ( f ) ( g ) : = P ( f e i ) ( g f j )

is a support-decreasing linear map P i j : C c ( V ) C c ( V ) . By the original result [29], there exists a discrete set Λ i j V V such that P i j is continuous on V Λ i j V , and every p V Λ i j V admits a neighbourhood U i j such that

P i j ( f ) ( g ) = σ N n ( σ f ) T i j σ ( g )

for all f , g C c ( U i j Λ i j V ) . Then 𝑃 is continuous on M Λ for the discrete set Λ = Λ i j V . For p M Λ , we can find a coordinate neighbourhood U = U i j such that, with

P ( s ) ( t ) = i j P i j ( s i ) ( t j ) for all s Γ c ( E | U ) and t Γ c ( F | U ) ,

the result follows with T i σ ( t ) = j T i j σ ( t j ) for t Γ c ( F | U ) . ∎

The above characterisation allows us to formulate a coordinate-free description of (distribution-valued) differential operators.

Definition C.2

We call a support-decreasing linear map P : Γ c ( E ) Γ c ( F ) a differential operator (of locally finite order) if Λ = , i.e. if 𝑃 is continuous.

Any support-decreasing continuous operator P : Γ ( E ) Γ c ( F ) induces a differential operator by restriction to Γ c ( E ) Γ ( E ) . However, for differential operators, the opposite is also true.

Lemma C.3

Let P : Γ c ( E ) Γ c ( F ) be a differential operator. Then 𝑃 induces a continuous morphism of sheaves E E D F , where E E ( U ) = Γ ( E | U ) and D F ( U ) = Γ c ( F | U ) . In particular, it induces a continuous map Γ ( E ) Γ c ( F ) .

Proof

This is stated in [29]; however, we will provide here a short explanation. First of all, for any U M , 𝑃 can be restricted to a continuous operator P U : Γ c ( E | U ) Γ c ( F | U ) by the natural extension Γ c ( E | U ) Γ c ( E ) and restriction Γ c ( F ) Γ c ( F | U ) . The resulting operator is still support-decreasing, so we only need to show extendibility from Γ c ( E | U ) to Γ ( E | U ) .

Given s Γ ( E | U ) and compact K U , any f K C c ( U ) with f K | K = 1 yields the same continuous linear functional P U ( f K s ) Γ K ( F | U ) , where Γ K denotes sections with support in 𝐾. This defines an element in the continuous linear dual of the locally convex injective limit Γ c ( F | U ) = lim Γ K ( F | U ) , denoted again by P U ( s ) . We get a support-decreasing operator P U : Γ ( E | U ) Γ c ( F | U ) that extends the originally given one. It is continuous since, for every compact K M , the composition of P U with the projection Γ c ( F | U ) Γ K ( F | U ) is continuous. ∎

We can now turn to the Poincaré Lemma for differential operators.

Lemma C.4

Let U R n be connected and open, and let E U be a vector bundle. For k 1 , let D : Ω c k ( U ) E = Γ c ( E ) be a differential operator (of locally finite order) with D d = 0 . Then there exists a differential operator Q : Ω c k + 1 ( U ) E such that D = Q d ,

Proof

First, note that 𝐷 uniquely extends from Ω c k ( U ) to Ω k ( U ) by Lemma C.3. We will work with this extension and note that it vanishes on all exact forms d Ω k 1 ( U ) , since Ω c k 1 ( U ) is dense in Ω k 1 ( U ) .

Let Ω k ( U ) denote the space of differential 𝑘-forms with polynomial coefficients of degree ℓ and Ω k ( U ) the space of differential 𝑘-forms with polynomial coefficients of degree at most ℓ. We construct inductively differential operators D : Ω k ( U ) E of order ℓ and Q : Ω k + 1 ( U ) E of order 1 such that

  1. D = Q d ,

  2. D D vanishes on Ω k ( U ) .

We start with D 0 = 0 and correspondingly Q 0 = 0 , because 𝐷 vanishes on differential 𝑘-forms with constant coefficients: Ω 0 k ( U ) = Ω 0 k ( V ) d Ω 1 k 1 ( U ) .

Let E = μ = 1 n x μ μ be the Euler vector field. Given a differential operator D of order ℓ which satisfies (1) and (2), we define the following differential operators of order + 1 :

D + 1 := D + 1 k + + 1 [ ( D D ) ι E ] d , Q + 1 := Q + 1 k + + 1 [ ( D D ) ι E ] .

Here [ A ] denotes the part of the differential operator 𝐴 which is of degree at most ℓ.[1] This notion is not coordinate-invariant, but that does not cause any problem for the proof, since we work in a fixed coordinate system. By construction and induction hypothesis, property (1), i.e. D + 1 = Q + 1 d , is satisfied.

Let us verify property (2). If α Ω + 1 k ( U ) , then d α Ω k + 1 ( U ) and

1 k + + 1 [ ( D D ) ι E ] > d α = 0 .

This means that [ ( D D ) ι E ] d α is equal to ( D D ) ι E d α . Thus

( D D + 1 ) α = ( D D ) α 1 k + + 1 ( D D ) ι E d α = ( D D ) α 1 k + + 1 ( D D ) L E α ,

where in the last equality we use the fact that ( D D ) d = D d D d = 0 . Now property (2) holds

  • for α Ω + 1 k ( U ) because L E α = ( k + + 1 ) α ,

  • and for α Ω k ( U ) because L E α Ω k ( U ) and D D vanishes on the subspace Ω k ( U ) .

On any precompact open set V U , the order of 𝐷 is bounded by some ℓ. There, we have D | V = D | V , since a differential operator of order ℓ is completely determined by what it does on polynomials of degree at most 𝑙. Consequently, we have Q + i | V = Q | V for all i 0 . This already implies that Q = lim Q | Ω c k + 1 ( U ) is a support-decreasing operator Ω c k + 1 ( U ) E . Moreover, 𝑄 is continuous, since it is locally continuous, i.e. it is a differential operator. ∎

Acknowledgements

The authors would like to thank Claude Roger for valuable insights into the history of the problem and Peter Kristel, Karl-Hermann Neeb, and Milan Niestijl for interesting discussions related to the project. The authors also thank the anonymous referee for their careful reading of the manuscript. Part of the work was carried out during a research stay of the authors at the Erwin Schrödinger International Institute for Mathematics and Physics, specifically during the program Higher Structures and Field-Theory.

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Received: 2024-11-01
Published Online: 2025-08-23
Published in Print: 2025-10-01

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