Exploring the Structure of Higher Algebroids

The notion of a \emph{higher-order algebroid}, as introduced in \cite{MJ_MR_HA_comorph_2018}, generalizes the concepts of a higher-order tangent bundle $\tau^k_M: \mathrm{T}^k M \rightarrow M$ and a (Lie) algebroid. This idea is based on a (vector bundle) comorphism approach to (Lie) algebroids and the reduction procedure of homotopies from the level of Lie groupoids to that of Lie algebroids. In brief, an alternative description of a Lie algebroid $(A, [\cdot, \cdot], \sharp)$ is a vector bundle comorphism $\kappa$ defined as the dual of the Poisson map $\varepsilon: \mathrm{T}^\ast A \rightarrow \mathrm{T} A^\ast$ associated with the Lie algebroid $A$. The framework of comorphisms has proven to be a suitable language for describing higher-order analogues of Lie algebroids from the perspective of the role played by (Lie) algebroids in geometric mechanics. In this work, we uncover the classical algebraic structures underlying the mysterious description of higher-order algebroids through comorphisms. For the case where $k=2$, we establish one-to-one correspondence between higher-order Lie algebroids and pairs consisting of a two-term representation (up to homotopy) of a Lie algebroid and a morphism to the adjoint representation of this algebroid.