The notion of coalgebra symmetry in Hamiltonian systems is analysed. It is
shown how the complete integrability of some long-range interacting Hamilto
nians can be extracted from their associated coalgebra structure with no us
e of a quantum R-matrix. Within this framework, integrable deformations can
be considered as direct consequences of the introduction of coalgebra defo
rmations (quantum algebras). As an example, the Gaudin magnet is derived fr
om a sl(2) coalgebra, and a completely integrable deformation of this Hamil
tonian is obtained through a twisted gl(2) quantum algebra.