We demonstrate that the anisotropy of the low-field critical point (H lcp ) of the vortex lattice melting line in a twinned YBa 2 Cu 3 O 7Ϫ␦ single crystal follows the intrinsic anisotropic behavior of the melting line when the disordered phase is originated by point defects. When the vortices are pinned at twin boundaries an upwards shift of H lcp is observed. The contribution of twin boundary pinning has been found to match with the change in the vortex elastic energy barriers thus supporting the identification of the low-field phase as a disordered solid vortex phase where vortex pinning overcomes the vortex-vortex interaction.In clean superconducting crystals the vortices present a first-order transition from a liquid to an ordered solid state. This transition has been characterized by several authors by means of thermodynamic, 1 magnetic, 2 and transport 3 measurements. When some kind of disorder is introduced in the lattice, however, a complex behavior appears which is controlled by the balance between vortex-vortex interaction, the pinning energy with defects, and thermal activation. One important consequence of disorder is that the lattice melting line is actually bounded by an upper critical field H ucp and a low critical field H lcp where the transition becomes second order. The influence of random point defects, such as oxygen vacancies, 4 electron or proton irradiation, 5 planar defects such as twin boundaries, 6,7 and columnar defects generated by ion irradiation, 8 on the features of the magnetic phase diagram of YBa 2 Cu 3 O 7Ϫ␦ , has been widely investigated, however a coherent picture is still lacking. The nature of the transition among the liquid and solid vortex states below the low-field critical point remains still an open issue. 9 In particular, the anisotropy of H lcp and its dependence on the different types of defects are not known. The low critical field may be shifted by more than two orders of magnitude, when the crystal is irradiated with protons. 5 When point defects are created by electron irradiation, however, the low-field critical point remains insensible. The influence of twin boundaries remains also extremely puzzling. 4,6,10 It was suggested that H lcp was not modified by twin boundaries but this is an unexpected behavior because twin boundaries lead to a secondorder Bose-glass transition, 11 characterized by a cusp in the ''irreversibility line'' and in the vortex activation energy for magnetic-field orientations close to the c axis. 12,13 This behavior would be also inconsistent with a recent study of the influence on H lcp of linear defects created by ion irradiation. 8 That work showed that H lcp is pushed up while the Boseglass regime develops. It appears then a fundamental problem to determine the intrinsic anisotropy of the critical points and their interaction with planar defects behaving as correlated disorder. 14 In this paper we address these fundamental open questions for the low-field critical point. From anisotropic magnetoresistance measurements we determine the...