Math 2.0

Global analysis, analysis on manifolds Definition

Schouten–Nijenhuis bracket

Builds on Smooth manifoldVector fieldLie bracket of vector fieldsLie derivativeExterior algebraPoisson manifold

Definition

Let MM be a smooth manifold. For p≥0p \ge 0, let 𝔛p(M)\mathfrak{X}^p(M) be the space of pp-vector fields, the smooth sections of the exterior power ΛpTM\Lambda^p TM. So 𝔛0(M)=C∞(M)\mathfrak{X}^0(M) = C^\infty(M), and 𝔛1(M)\mathfrak{X}^1(M) is the space of vector fields. The Schouten–Nijenhuis bracket is the unique family of ℝ\R-bilinear maps [⋅,⋅] ⁣:𝔛p(M)×𝔛q(M)→𝔛p+q−1(M)[\cdot, \cdot] \colon \mathfrak{X}^p(M) \times \mathfrak{X}^q(M) \to \mathfrak{X}^{p+q-1}(M) with these properties, for P∈𝔛p(M)P \in \mathfrak{X}^p(M), Q∈𝔛q(M)Q \in \mathfrak{X}^q(M) and R∈𝔛r(M)R \in \mathfrak{X}^r(M).

  1. For functions f,gf, g: [f,g]=0[f, g] = 0.
  2. For a vector field XX: [X,P]=ℒXP[X, P] = \mathcal{L}_X P, the Lie derivative; in particular [X,f]=X(f)[X, f] = X(f) and [X,Y][X, Y] is the Lie bracket.
  3. Graded antisymmetry: [P,Q]=−(−1)(p−1)(q−1)[Q,P][P, Q] = -(-1)^{(p-1)(q-1)} [Q, P].
  4. Graded Leibniz rule: [P,Q∧R]=[P,Q]∧R+(−1)(p−1)q Q∧[P,R][P, Q \wedge R] = [P, Q] \wedge R + (-1)^{(p-1)q}\, Q \wedge [P, R].

Remarks

For vector fields X1,…,XpX_1, \dots, X_p and Y1,…,YqY_1, \dots, Y_q with p,q≥1p, q \ge 1, the bracket is [X1∧⋯∧Xp, Y1∧⋯∧Yq]=∑i=1p∑j=1q(−1)i+j[Xi,Yj]∧X1∧…Xi^⋯∧Xp∧Y1∧…Yj^⋯∧Yq,[X_1 \wedge \dots \wedge X_p,\ Y_1 \wedge \dots \wedge Y_q] = \sum_{i=1}^{p} \sum_{j=1}^{q} (-1)^{i+j} [X_i, Y_j] \wedge X_1 \wedge \dots \widehat{X_i} \dots \wedge X_p \wedge Y_1 \wedge \dots \widehat{Y_j} \dots \wedge Y_q, where a hat marks an omitted factor. The bracket also satisfies a graded Jacobi identity, so 𝔛∙+1(M)\mathfrak{X}^{\bullet + 1}(M), with degrees shifted by one, is a graded Lie algebra.

A bivector field π∈𝔛2(M)\pi \in \mathfrak{X}^2(M) defines the bracket {f,g}=π(df,dg)\{f, g\} = \pi(df, dg) on functions. This bracket satisfies the Jacobi identity, so that π\pi is a Poisson structure, exactly when [π,π]=0[\pi, \pi] = 0.

Example: on ℝ2\R^2, let π=∂x∧∂y\pi = \partial_x \wedge \partial_y. All brackets of the coordinate vector fields vanish, so the formula gives [π,π]=0[\pi, \pi] = 0, and {f,g}=fxgy−fygx\{f, g\} = f_x g_y - f_y g_x is the standard Poisson bracket.

Non-example: the wedge product (P,Q)↦P∧Q(P, Q) \mapsto P \wedge Q is bilinear but is not this bracket. It fails property 2: for a vector field XX and a function ff, it gives X∧f=fXX \wedge f = fX, while property 2 requires the function X(f)X(f).

Reading path

To understand this page from the ground up, read these 10 pages in order. The foundations come first.

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  1. Euclidean space object
  2. Exterior algebra concept
  3. Function concept
  4. Lie bracket of vector fields concept
  5. Lie derivative concept
  6. Poisson manifold concept
  7. Smooth manifold concept
  8. Vector-valued function concept
  9. Vector field concept
  10. Schouten–Nijenhuis bracket definition

Further reading

  1. Web https://en.wikipedia.org/wiki/Schouten%E2%80%93Nijenhuis_bracket
About this page
TagE5G2SSTBP3
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Kinddefinition
WritingW0 stub
MSC58A10, 17B70, 53D17
DefinesSchouten–Nijenhuis bracket
UsesSmooth manifold, Vector field, Lie bracket of vector fields, Lie derivative, Exterior algebra, Poisson manifold

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