Using the valence-bond-solid (VBS) approach and the Schwinger-boson mean-field approximation, we study the dependence of the Haldane gap of a spin-1 linear-chain Heisenberg antiferromagnet on impurity doping with different spins. The impurity spins affect the singlet pairing order parameter \ensuremath{\Delta} and the constraint factor \ensuremath{\lambda}. As a result, the Haldane gap is reduced by a factor \ensuremath{\sim}
ni2/3, with
ni as the impurity concentration, and eventually collapses at
ni\ensuremath{\sim}1/\ensuremath{\xi} with \ensuremath{\xi} as the VBS correlation length. This theoretical prediction can be verified by neutron-scattering experiments.
We study the long-wavelength limit of a spin
S Heisenberg antiferromagnetic chain. The fermionic Lagrangian obtained corresponds to a perturbed level
2S SU(2) Wess-Zumino-Witten (WZW) model. This effective theory is then mapped into a compact
U(1) boson interacting with
Z2S parafermions. The analysis of this effective theory allows us to show that when
S is an integer there is a mass gap to all excitations, whereas this gap vanishes in the half-odd-integer spin case and the
SU(2)2S WZW model flows towards the
SU(2)1 stable fixed point. This gives a field theory treatment of the so-called Haldane's conjecture for arbitrary values of the spin
S.
Motivated by recent experiments on low-dimensional quantum magnets in applied magnetic fields, we present a theoretical analysis of their properties based on the nonlinear sigma model. The spin stiffness and a 1/N expansion are used to map the regimes of spin-gap behavior, predominantly linear magnetization, and spin saturation. A two-parameter renormalization-group study gives the characteristic properties over the entire parameter range. The model is relevant to many systems exhibiting Haldane physics, and is applied here to the two-chain spin ladder compound CuHpCl.