We demonstrate that the variation of the Andreev reflection with applied magnetic field provides a direct means of comparing the properties of MgB 2 with the theory for a dirty two-band superconductor, and we find good agreement between the two. The ratio of electron diffusivities in the σ and π bands can be inferred from this experiment. We find that the field dependence of the density of states at the Fermi level in the π band is independent of the field direction, and that the anisotropic upper critical field is determined by the anisotropic diffusivity in the σ band. ) will change the resulting macroscopic superconducting properties, and therefore independent determination of this ratio has emerged as a key prerequisite to understand and control the properties of MgB 2 . Due to the crystalline anisotropy, the diffusivities along the c axis ( ). It is in principle possible to obtain the scattering rates from the temperature dependence of the resistivity [7,8], but this method is subject to large uncertainty if the sample is not 100% dense [9], which is often the case with MgB 2 . In this work we demonstrate that the diffusivity ratio can be directly evaluated from point-contact Andreev reflection (PCAR) spectroscopy in magnetic field.Point-contact [10,11,12] and tunnelling spectroscopies [13,14], have been used to study the properties of MgB 2 in applied magnetic field. The scanning tunneling spectroscopy (STS) images of vortices parallel to the c axis [13] have been successfully explained by theory [4]. Importantly, vortex imaging is demanding experimentally and probes mainly the properties of the π band. It is possible to use the STS method to probe the in-plane vortices in sufficiently thick single crystals [14], but certainly not in thin films. The effect of vortices on the point-contact measurements has not been considered.In our previous work [15] we have demonstrated that as the field is increased, the transition to the normal state occurs simultaneously in the two superconducting sub-systems, i.e., the σ and π bands are characterised by a unique H c2 . Later we have studied the evolution of the PCAR spectra with magnetic field in niobium [16]; we showed that the mechanism behind the field variation of the Andreev reflection in Type-II superconductor is the presence of normal vortex cores, which leads to effective broadening of the spectra and increasing the zero-energy density of states (DOS), N 0 (corresponding