We show by neutron diÃraction that metallic V2 "03develops a spin density wave below T~= 9 K with incommensurate wave vector g 1. 7c* and an ordered moment of 0.15@,. The weak ordering phenomenon is accompanied by strong, nonresonant spin fluctuations with a velocity c = 67 (4) We grew single crystals of V2 &Os using a skull melter [6]. The cation deficiency was controlled to within by=0. 003 by annealing 2 mm thick slabs for two weeks at 1400'C in a CO-CO2 atmosphere [7]. Four single crystals with a total volume of 7 cm3 were sliced into comb shapes prior to annealing for use in the inelastic experi- (h0l) zones. High pressure neutron difFraction was performed using a maraging steel cell with 4He as the pressure transducing medium.We first characterized the low temperature (T = 1.4 K) antiferromagnetic phase in metallic V2 "Os [2,8]. Antiferrornagnetic Bragg peaks were not found at (2 20), corresponding to the ordered structure of the insulator, but instead appeared as pairs at incommensurate positions (h0l + h) with b = 1.7 and for l -4h = Gn. In Fig. 1 we show the incommensurate peaks corresponding to (102+ 6') and (104 -h' ) from which we find 6 = 1.700(2) for y = 0.037(4). The peaks are resolution limited placing a lower limit of 10s A. on the correlation length, (. Extensive searches along high symmetry directions in the (hOl) zone revealed no other temperature dependent Bragg peaks. These observations imply the presence of a static spin configuration which may be described as SR, g = S x cos(q R+ pd) + S"ysin(q R+ p~), where x and y are orthogonal unit vectors and R is a Bravais lattice vector. In order to determine the phases P~o f the four magnetic ions within a primitive unit cell and the size of the ordered moment, we measured the integrated intensities of 13 magnetic satellites. Absolute units were derived by normalizing to 22