[1.86]
where:
[1.87]
where
The other pre-Lie operation ⊲ of section 1.6.1.2, more precisely its opposite ⊳, is associated with another right-sided Hopf algebra of forests ℋ which has been investigated in Calaque et al. (2011) and Manchon and Saidi (2011), and which can be defined by considering trees as Feynman diagrams (without loops): let
Let s be a subforest of a rooted tree t. Denote by t/s the tree obtained by contracting each connected component of s onto a vertex. We turn ℋ into a bialgebra by defining a coproduct Δ : ℋ → ℋ ⊗ ℋ on each tree
[1.88]
where the sum runs over all possible subforests (including the unit • and the full subforest t). As usual we extend the coproduct Δ multiplicatively onto
[1.89]
[1.90]
It turns out that ℋCK is left comodule-bialgebra over ℋ (Calaque et al. 2011; Manchon and Saidi 2011), in the sense that the following diagram commutes:
Here, the coaction Φ : ℋCK → ℋ ⊗ ℋCK is the algebra morphism given by Φ(1) = • ⊗ 1 and Φ(t) = Δℋ(t) for any nonempty tree t. As a result, the group of characters of ℋ acts on the group of characters of ℋCK by automorphisms.
1.6.4. Pre-Lie algebras of vector fields
1.6.4.1. Flat torsion-free connections
Let M be a differentiable manifold, and let ▽ be the covariant derivation operator associated with a connection on the tangent bundle TM. The covariant derivation is a bilinear operator on vector fields (i.e. two sections of the tangent bundle): (X, Y) ↦ ▽XY, such that the following axioms are fulfilled:
The torsion of the connection
is defined by: [1.91]
and the curvature tensor is defined by:
[1.92]
The connection is flat if the curvature R vanishes identically, and torsion-free if
PROPOSITION 1.14.– For any smooth manifold M endowed with aflat torsion-free connection ▽, the space χ(M) of vector fields is a left pre-Lie algebra, with pre-Lie product given by:
[1.93]
Note that on M = ℝn, endowed with its canonical flat torsion-free connection, the pre-Lie product is given by:
1.6.4.2. Relating two pre-Lie structures
Cayley (1857) discovered a link between rooted trees and vector fields on the manifold ℝn, endowed with its natural flat torsion free connection, which can be described in modern terms as follows: let
PROPOSITION 1.15.– For any rooted tree t, with each vertex v being decorated by a vector field Xv, the vector field
[1.95]