In this article we review recent developments in the one-dimensional Bethe
ansatz solvable multi-chain quantum models. The algebraic version of the Be
the ansatz (the quantum inverse scattering method) permits us to construct
new families of integrable Hamiltonians using simple generalizations of the
well known constructions of the single-chain model. First we consider the
easiest example ('basic' model) of this class of models: the antiferromagne
tic two-chain spin-1/2 model with the nearest-neighbour and next-nearest-ne
ighbour spin- frustrating interactions (zigzag chain). We show how the alge
bra of the quantum inverse scattering method works for this model, and what
are the important features of the Hamiltonian (which reveal the topologica
l properties of two dimensions together with the one-dimensional properties
). We consider the solution of the Bethe ansatz for the ground state (in pa
rticular, commensurate-incommensurate quantum phase transitions present due
to competing spin-frustrating interactions are discussed) and construct th
e thermal Bethe ansatz (in the form of the 'quantum transfer matrix') for t
his model. Then possible generalizations of the basic model are considered:
an inclusion of a magnetic anisotropy. higher-spin representations (includ
ing the important case of a quantum ferrimagnet), the multi-chain case, int
ernal degrees of freedom of particles at each site, etc. We observe the sim
ilarities and differences between this class of models and related exactly
solvable models: other groups of multi-chain lattice models, quantum field
theory models and magnetic impurity (Kondo-like) models. Finally, the behav
iour of non-integrable (less constrained) multi-chain quantum models is dis
cussed.