The two-time Green's function method is used to study the critical properties and crossover phenomena near the field-induced quantum critical point (QCP) of a
d-dimensional spin-
S planar Heisenberg ferromagnet with long-range interactions decaying as ${r}^{\ensuremath{-}\ensuremath{\alpha}}$ (with $\ensuremath{\alpha}>d$) with the distance
r between spins. We adopt the Callen scheme for spin
S and the Tyablikov decoupling procedure which is expected to provide suitable results at low temperatures. Different quantum critical regimes are found in the $(\ensuremath{\alpha},d)$ plane and the global structure of the phase diagram is determined showing the typical V-shaped region close to the QCP. Depending on the values of $\ensuremath{\alpha}$, we find that also for dimensionalities $d\ensuremath{\leqslant}2$ a finite-temperature critical line, ending in the QCP, exists with asymptotic behaviors and crossovers which can be employed as a useful guide for experimental studies. Moreover, these crossovers are shown to be suitably described in terms of $(\ensuremath{\alpha},d)$-dependent scaling functions and effective critical exponents.
Critical dynamics of planar ferromagnet with a small basal plane anisotropy is considered as an example in which the crossover from the planar limit to the anisotropic limit can be studied with the ε-expansion technique where ε= 4-d, d being the dimensionality of space. Explicit expressions are given for the decay rates of the three components of spins at criticality for q ≫Δ1/2 and q ≪Δ1/2 as well as in the limit ε→0 where q and Δ are the wave number and the size of the basal plane anisotropy, respectively.