Nuclear magnetic resonance (NMR) study of the high magnetic field (H) part of the Bose-Einstein condensed (BEC) phase of the quasi-onedimensional (quasi-1D) antiferromagnetic quantum spinchain compound NiCl2-4SC(NH2)2 (DTN) was performed. We precisely determined the phase boundary, Tc(H), down to 40 mK; the critical boson density, nc(Tc); and the absolute value of the BEC order parameter S ⊥ at very low temperature (T = 0.12 K). All results are accurately reproduced by numerical quantum Monte Carlo simulations of a realistic three-dimensional (3D) model Hamiltonian. Approximate analytical predictions based on the 1D Tomonaga-Luttinger liquid description are found to be precise for Tc(H), but less so for S ⊥ (H), which is more sensitive to the strength of 3D couplings, in particular close to the critical field. A mean-field treatment, based on the Hartree-Fock-Popov description, is found to be valid only up to nc ∼ = 4% (T < 0.3 K), while for higher nc boson interactions appear to modify the density of states.PACS numbers: 67.80.dk, 75.40.Mg, 75.40.Cx, 75.10.Jm Quantum phase transitions, i.e., phase transitions that are driven by quantum, rather than thermal, fluctuations, are one of the topical subjects in condensed matter physics. [1][2][3][4] There are numerous experimental investigations of such transitions as a function of an external control parameter, such as magnetic field (H), pressure, or chemical composition. The NiCl 2 -4SC(NH 2 ) 2 (DTN) quantum magnet has long been studied in this respect.5-11 The system consists of weakly coupled chains of S = 1 spins, borne by Ni 2+ ions, subject to the Hamiltonian where summations are performed over all lattice positions (r) and unit cell vectors (v). Equation (1) shows that the spins are subject to an easy-plane anisotropy [the D(Ŝ z r ) 2 term, where D/k B = 8.9 K] and the nearest-neighbor Heisenberg interaction (J vŜr ·Ŝ r+v ), preferentially along the chain (c-axis direction), J c /k B = 2.2 K. Also, an interchain coupling J ab /k B = 0.18 K is present, which, because of the tetragonal symmetry, is equivalent for the a and b directions. As the antiferromagnetic (AF) couplings differ by an order of magnitude (J c /J ab ∼ = 12), the system can be considered as quasi-onedimensional (quasi-1D). Between critical fields H c1 = 2.1 T and H c2 = 12.32 T, 6,7,9 and at low temperature (T ) it displays a three-dimensional (3D) AF ordered phase that can be described as a Bose-Einstein condensation (BEC) of the spin degrees of freedom (belonging to the 3D XY universality class).12 In the BEC phase a transverse AF magnetic moment develops, corresponding to the BEC order parameter.12-15 Although the existence of such a state is intrinsically a 3D phenomenon, a pronounced 1D character is known to affect some of its properties in a nontrivial and interesting way. 16,17 The spin ladders CuBr 4 (C 5 H 12 N) 2 (BPCB) 17,18 and (C 7 H 10 N 2 )CuBr 4 (DIMPY), 19-21 whose anisotropy of coupling constants (1D character) is ∼10 times stronger than in DTN, were successfully descr...