A new numerical method is proposed for a 1-D inverse medium scattering problem with multi-frequency data. This method is based on the construction of a weighted cost functional. The weight is a Carleman Weight Function (CWF). In other words, this is the function, which is present in the Carleman estimate for the undelying differential operator. The presence of the CWF makes this functional strictly convex on any a priori chosen ball with the center at {0} in an appropriate Hilbert space. Convergence of the gradient minimization method to the exact solution starting from any point of that ball is proven. Computational results for both computationally simulated and experimental data show a good accuracy of this method. of [11], which is based on Carleman estimates and which was originally designed in [11] only for proofs of uniqueness theorems for CIPs, also see the recent survey in [27].Another version of the GCM with a CWF in it was recently developed in [6] for a CIP for the hyperbolic equation w tt = ∆w + a (x) w + f (x, t) , where a (x) is the unknown coefficient. This GCM was tested numerically in [7]. In [6,7] non-vanishing conditions are imposed: it is assumed that either f (x, 0) = 0 or w (x, 0) = 0 or w t (x, 0) = 0 in the entire domain of interest. Similar assumptions are imposed in [10,29] for the GCM of the second type. On the other hand, we consider in the current paper, so as in [24,25,26,33], the fundamental solution of the corresponding PDE. The differences between the fundamental solutions of those PDEs and solutions satisfying non-vanishing conditions cause quite significant differences between [24, 25, 26, 33] and [6, 7, 10, 29] of corresponding versions of the GCM of the second type.Recently, the idea of the GCM of the second type was extended to the case of ill-posed Cauchy problems for quasilinear PDEs, see the theory in [28] and some extensions and numerical examples in [4,30].CIPs of wave propagation are a part of a bigger subfield, Inverse Scattering Problems (ISPs). ISPs attract a significant attention of the scientific community. In this regard we refer to some direct methods which successfully reconstruct positions, sizes and shapes of scatterers without iterations [12,13,20,22,36,37,38,45]. We also refer to [3,37,41,42] for some other ISPs in the frequency domain. In addition, we cite some other numerical methods for ISPs considered in [2,5,46].As to the CIPs with multiple measurement, i.e. the Dirichlet-to-Neumann map data, we mention recent works [1,21,43] and references cited therein, where reconstruction