nLab volume preserving diffeomorphism

Redirected from "volume-preserving diffeomorphisms".

Contents

Idea

A diffeomorphism ϕ:XX\phi \colon X \longrightarrow X of a (pseudo-) Riemannian manifold XX is volume preserving (VPD) if its pullback of differential forms fixes the volume form: ϕ *vol=vol\phi^\ast vol = vol.

If the dimension is dim(X)=2dim(X) = 2, then one also speaks of area-preserving diffeomorphisms (APD).

Properties

Volume preserving diffeomorphisms form a topological subgroup

SDiff(X)Diff(X) + SDiff(X) \subset Diff(X)^+

of the general (orientation-preserving) diffeomorphism group of the underlying smooth manifold of XX.

Proposition

This inclusion is a weak homotopy equivalence, in fact a deformation retract.

This follows by Moser's theorem (cf. Banyaga 1997 Cor. 1.5.4).

For XX compact, SDiffSDiff is an infinite-dimensional Fréchet Lie group.

Its Lie algebra then is the algebra of incompressible (i.e. zero-divergence) vector fields on XX. For the case dim(X)=2dim(X) = 2, these Lie algebras (or their central extensions) are known as w w_\infty -algebras (with lower case “w”) and certain deformation quantizations of these as W W_\infty -algebras (with capital “W”).

In physics

In physics (field theory), volume-preserving diffeomorphisms appear:

But beware that most of the physics literature considers this at the level of Lie algebras, which can be misleading as the relation of infinite-dimensional Lie groups to their Lie algebras is more loose. For instance:

References

General

Monograph:

Original discussion of the w w_\infty -algebra of the torus:

  • Vladimir Arnold; equation (109) in: Sur la géométrie différentielle des groupes de Lie de dimension infinie et ses applications à l’hydrodynamique des fluides parfaits, Annales de l’Institut Fourier 16 1 (1966) 319–361 [numdam:AIF_1966__16_1_319_0/]

Proof that the volume-preserving diffeomorphism group of Cartesian space n\mathbb{R}^n is a perfect group when n3n \geq 3:

Discussion in relation to w w_\infty -algebras:

Linear representations

There is no general representation theory of VPDs, but (cf. Pickrell 2000 p. 179) the following examples of linear representations of SDiffSDiff have been constructed.

Reps of SDiff( 3)SDiff(\mathbb{R}^3)

In the context of discussion of vortices:

Reps of SDiff(S 2)SDiff(S^2)

Representation on sections of determinant line bundles of (tacitly) 3D Maxwell-Chern-Simons theory:

using a rigorous APD-invariant path integral measure for 2D Yang-Mills theory, due to:

In the context of the Plebański formulation of gravity:

Via the orbit method:

Relation between 𝔰𝔲()\mathfrak{su}(\infty) and Lie(SDiff(Σ))Lie(SDiff(\Sigma))

On the identification of the special unitary Lie algebra 𝔰𝔲 ( n ) \mathfrak{su}(n) , as nn \to \infty, with the Lie algebra of area-preserving diffeomorphisms of surfaces Σ\Sigma (cf. also at Quantization of the M2-brane to the BFSS matrix model):

For the 2-sphere:

For the 2-torus:

Warning that the analogous statements for the Lie groups (as opposed to their Lie algebras) fail dramatically, for basic topological reasons:

  • John Swain: On the limiting procedure by which SDiff(T 2)SDiff(T^2) and SU()SU(\infty) are associated [arXiv:hep-th/0405002]

  • John Swain: The Topology of SU()SU(\infty) and the Group of Area-Preserving Diffeomorphisms of a Compact 2-manifold [arXiv:hep-th/0405003]

  • John Swain: The Majorana representation of spins and the relation between SU()SU(\infty) and SDiff(S 2)SDiff(S^2) [arXiv:hep-th/0405004]

Analogous discussions:

for the tetrahedron:

  • A. Wolski, J. S. Dowker: Area‐preserving diffeomorphisms of the tetrahedron, J. Math. Phys. 32 (1991) 857–863 [doi:10.1063/1.529343]

for 𝔰𝔩 ( n ; ) \mathfrak{sl}(n;\mathbb{N}) and 𝔰𝔲(n,n)\mathfrak{su}(n,n):

and in relation to the KP hierarchy:

As symmetries of brane dynamics

On volume-preserving diffeomorphisms as residual gauge symmetries of brane sigma-models in light cone gauge:

On APD symmetry of the M2-brane sigma-model (cf. M2-brane – Light-cone quantization to the BFSS matrix model):

and on VPD symmetry in the M2’s covariant formulation:

  • So Katagiri: A Lorentz Covariant Matrix Model for Bosonic M2-Branes: Nambu Brackets and Restricted Volume-Preserving Deformations [arXiv2504.05940]

  • So Katagiri: Quantum Stability at One Loop for BPS Membranes in a Lorentz-Covariant RVPD Matrix Model [arXiv:2509.23853]

Generalization to light cone gauge VPD symmetry of the higher-dimensional super p-branes without gauge fields on their worldvolume:

See also:

  • Y. Matsuo, Y. Shibusa: Volume Preserving Diffeomorphism and Noncommutative Branes, JHEP 0102:006 (2001) [arXiv:hep-th/0010040]

On VPD symmetry in the Nambu-Poisson M5-brane model:

Review:

On VPD symmetry of the actual M5-brane sigma-model:

See also:

As symmetries of fractional quantum Hall systems

As (gauge) symmetries of fractional quantum Hall systems (cf. supersymmetry in FQH systems and for more see at W W_\infty -algebra):

Analog for 3d VPDs:

  • Giandomenico Palumbo: Generalized GMP Algebra for Three-Dimensional Quantum Hall Fluids of Extended Objects [arXiv:2602.15664]

Last revised on April 8, 2026 at 16:11:40. See the history of this page for a list of all contributions to it.