Abstract
We provide the explicit solution of the n-dimensional generalised ladder system, that is the homogeneous quadratic system of first-order differential equations of the form \\dotxi=xi∑j=1naijxj, i=1,n, where (aij)=(1+ai−aj), i,j=1,n introduced by Imai and Hirata [J. Phys. Soc. Jpn. 72 (2003) 973]. These systems are characterised by the n2−1 symmetries Yml=xmual−am−1(∑j=1nxj∂xj−u∂xl), but are not the most general systems invariant under these symmetries. The more general systems are called hyperladder systems and we discuss their integrability.