We provide arguments in favour of impact origin of a 200 km suspected impact crater Kotuykanskaya near Popigai, Siberia, Russia. We use the gravity aspects (gravity disturbances, the Marussi tensor of the second derivatives of the disturbing geopotential, the gravity invariants and their specific ratio, the strike angles and the virtual deformations), all derived from the combined static gravity field model EIGEN 6C4, with the ground resolution of about 10 km and a precision of about 10 milliGals. We also use the magnetic anomalies from the model EMAG2 and emphasize the evidence of much deeper sources in the suspected area, constraining the impact origin of this structure. Motivation, method, theory, and data. Motivation. The objective of this study is to use recently available high-resolution gravity aspects (descriptors) derived from the global Earth's gravity field model EIGEN 6C4 1 with the ground resolution of about 9 km, to provide an independent assessment of the existence of a suspected Kotuykanskaya impact crater(s) near the proven impact crater Popigai in Siberia, Russia.It would be one of the largest impact craters on the Earth -with a diameter of ~200 km, about twice as large as Popigai, comparable to Chicxulub, so it is worthy to study it when we have available new gravity data and a new methodology (see comments below). Nevertheless, we have no detailed geological data available, so we cannot provide any final decision.For the given locality our aim is to apply the new available gravity aspects (derived from EIGEN 6C4), magnetic anomalies (EMAG v. 2) and surface topography (ETOPO 1).Methodology. Classical gravity anomalies (or disturbances Δg) provide only limited information about the stress state of the rocks causing them. In order to broaden the potential information about the state of rocks we compute various gravity functions (the gravity aspects) of the disturbing gravitational potential expressed in the spherical harmonic expansion to a high degree and order (known as the geopotential coefficients or the Stokes parameters) in addition to the gravity anomalies Δg. The core of our method is in the use of various gravitational aspects, namely the components of the Marussi tensor Γ of the second derivatives T ij of the disturbing potential, the gravity invariants I 1 and I 2 , their specific ratio I, the strike angles θ and the virtual deformations vd. Each of these gravity aspect tells its own "story" about the density due to the causative body and in turn about the gravity signal generated.Comments to theory.