We present spatial and dynamic information on the s = 1/2 distorted kagome antiferromagnet volborthite, Cu 3 V 2 O 7 (OD) 2 · 2D 2 O, obtained by polarized and inelastic neutron scattering. The instantaneous structure factor, S(Q), is dominated by nearest-neighbor pair correlations, with short-range order at wave vectors Q 1 = 0.65(3)Å −1 and Q 2 = 1.15(5)Å −1 emerging below 5 K. The excitation spectrum, S(Q,ω), reveals two steep branches dispersing from Q 1 and Q 2 , and a flat mode at ω f = 5.0(2) meV. The results allow us to identify the crossover at T * ∼ 1 K in 51 V NMR and specific-heat measurements as the buildup of correlations at Q 1 . We compare our data to theoretical models proposed for volborthite, and also demonstrate that the excitation spectrum can be explained by spin-wave-like excitations with anisotropic exchange parameters, as suggested by recent local-density calculations. 2 The physics of herbertsmithite is arguably influenced by depletion of the kagome lattice caused by antisite mixing, possibly resulting in a valence bond glass state. 3,4 In volborthite, the kagome planes are slightly distorted, but the lattice coverage is essentially complete. Since both systems deviate from the pure QKHAF model, focus has shifted to the intriguing question of which states arise when the QKHAF is perturbed. Remarkably, a multitude of different states have been proposed theoretically, depending on the nature of the perturbation. These range from ordered states [5][6][7][8][9] to the aforementioned valence bond glass. Experimentally, the ground state of volborthite remains enigmatic, despite over ten years of intensive study.2,10-13 Here we present a neutron-scattering investigation of volborthite, employing both xyz-polarized and inelastic time-of-flight techniques.Volborthite contains distorted kagome planes of edgesharing Cu 2+ octahedra, well separated (∼ 7.2Å) by pyrovanadate columns (V 2 O 7 ), Fig. 1(a). There are two crystallographically distinct Cu 2+ ions: Cu(2) forms chains along the b direction, while Cu(1) populates the interchain sites. Locally, Cu(1) and Cu(2) reside in tetragonally and axially distorted octahedra, respectively, suggesting the d 3z 2 −r 2 orbital being singly occupied on the Cu(1) site, with d x 2 −y 2 the magnetically active orbital for Cu(2). As a consequence, there are two different nearest-neighbor exchange pathways, J 1 (r Cu(2)-Cu(2) = 2.93Å) and J 1 (r Cu(1)-Cu(2) = 3.03Å). J 1 links Cu(2) ions along the b axis, while J 1 connects Cu(1) and Cu(2) ions. Furthermore, the edge sharing of the Cu (2) octahedra along the b direction implies the possibility of a strong next-nearest-neighbor exchange, J 2 .Despite a large estimated average nearest neighbor coupling J avg = (2J 1 + J 1 )/3 = 84 K, magnetic susceptibility and specific-heat measurements on volborthite show no signs of long-range order down to 1.8 K 2 . At yet lower temperatures, muon spin rotation (μSR) and 51 V NMR (Refs. 10-12) indicate slowing down of fluctuations at T * = 1 K, but with dynamics persisting to...