Dirac structure

In mathematics a Dirac structure is a geometric construction generalizing both symplectic structures and Poisson structures, and having several applications to mechanics. It is based on the notion of constraint introduced by Paul Dirac and was first introduced by Ted Courant and Alan Weinstein.

In more detail, let V be a real vector space, and V* its dual. A Dirac structure on V is a linear subspace D of $V\times V^{*}$ satisfying

• for all $(v,\alpha )\in D$ one has $\left\langle \alpha ,\,v\right\rangle =0$,
• D is maximal with respect to this property.

In particular, if V is finite dimensional then the second criterion is satisfied if $\dim D=\dim V$. (Similar definitions can be made for vector spaces over other fields.)

An alternative (equivalent) definition often used is that $D$ satisfies $D=D^{\perp }$, where orthogonality is with respect to the symmetric bilinear form on $V\times V^{*}$ given by ${\bigl \langle }(u,\alpha ),\,(v,\beta ){\bigr \rangle }=\left\langle \alpha ,v\right\rangle +\left\langle \beta ,u\right\rangle .$

Examples:

1. If $U\subset V$ is a vector subspace, then $D=U\times U^{\circ }$ is a Dirac structure on $V$, where $U^{\circ }$ is the annihilator of $U$; that is, $U^{\circ }=\left\{\alpha \in V^{*}\mid \alpha _{\vert U}=0\right\}$.
2. Let $\omega :V\to V^{*}$ be a skew-symmetric linear map, then the graph of $\omega$ is a Dirac structure.
3. Similarly, if $\Pi :V^{*}\to V$ is a skew-symmetric linear map, then its graph is a Dirac structure.

A Dirac structure ${\mathfrak {D}}$ on a manifold M is an assignment of a Dirac structure on the tangent space to M at m, for each $m\in M$. That is,

• for each $m\in M$, a Dirac subspace $D_{m}$ of the space $T_{m}M\times T_{m}^{*}M$.

Many authors, in particular in geometry rather than the mechanics applications, require a Dirac structure to satisfy an extra integrability condition as follows:

• suppose $(X_{i},\alpha _{i})$ are sections of the Dirac bundle ($i=1,2,3$) then $\left\langle L_{X_{1}}(\alpha _{2}),\,X_{3}\right\rangle +\left\langle L_{X_{2}}(\alpha _{3}),\,X_{1}\right\rangle +\left\langle L_{X_{3}}(\alpha _{1}),\,X_{2}\right\rangle =0.$

In the mechanics literature this would be called a closed or integrable Dirac structure.

Comparison with symplectic and Poisson structures

Let $\omega$ be a symplectic form on a manifold $M$, then its graph is a (closed) Dirac structure. More generally this is true for any closed 2-form. If the 2-form is not closed then the resulting Dirac structure is not closed (integrable).

Let $\Pi$ be a Poisson structure on a manifold $M$, then its graph is a (closed) Dirac structure.

References

T. Courant, Dirac manifolds. Trans. American Math. Soc., 319: 631-661, 1990.

T. Courant and A. Weinstein: Beyond Poisson structures. Seminare sud-rhodanien de géométrie VIII. Travaux en Cours 27, Paris: Hermann, 1988

I. Ya Dorfman, Dirac structures and integrability of nonlinear evolution equations Chichester: Wiley, 1993

F. Gay-Balmaz and H. Yoshimura, Dirac structures in nonequilibrium thermodynamics for simple open systems. J. Math. Phys. 61 (2020), no. 9, 092701, 45 pp.

A.J. van der Schaft and B.M. Maschke, Hamiltonian formulation of distributed-parameter systems with boundary energy flow. Journal of Geometry and Physics, vol. 42, pp. 166{194, 2002.

H. Yoshimura and J.E. Marsden, Dirac structures in Lagrangian mechanics. I. Implicit Lagrangian systems. J. Geom. Phys. 57 (2006), 133–156.

H. Yoshimura and J.E. Marsden, Dirac structures in Lagrangian mechanics. II. Variational structures. J. Geom. Phys. 57 (2006), 209–250.