We discuss the one-loop quantum corrections to the mass M and central charge Z of supersymmetric (susy) solitons: the kink, the vortex and the monopole. Contrary to previous expectations and published results, in each of these cases there are nonvanishing quantum corrections to the mass. For the N = 1 kink and the N = 2 monopole a new anomaly in Z rescues BPS saturation (M = Z); for the N = 2 vortex, BPS saturation is rescued for two reasons: (i) the quantum fluctuations of the Higgs field acquire a nontrivial phase due to the winding of the classical solution, and (ii) a fermionic zero mode used in the literature is shown not to be normalizable. Solitons can be viewed as extended particles ("lumps") which should clearly have finite mass (= finite energy at rest). We shall only consider relativistic field theories. There exist also time-dependent solutions with finite energy (the "breather" solution in the sine-Gordon model, for example), but we consider only time-independent solitons. One can, of course, boost solitons in a relativistic theory, and obtain then moving solitons, but since one can always choose a Lorentz frame in which they are at rest, we restrict our attention to only time-independent solutions.A soliton is closely related to an instanton. The later is defined as follows:Definition 2: an instanton is a nonsingular solution of the classical field equations in Euclidean space with finite action.Because instantons have finite action, they contribute already at the classical level to the path integral. This is the reason for the requirement of finite action. It is clear that a soliton in n + 1 dimensions is an instanton in n dimensions: since the time coordinate plays no role in the soliton solutions, the space integral in Minkowski space can also be viewed as an integral over Euclidean space, and the energyWe shall discuss three solitons:1) the kink in 1+1 dimensions with N = 1 susy 2) the vortex in 2+1 dimensions with N = 2 susy 3) the monopole in 3+1 dimensions with N = 2 susyThere exist also susy extensions of these solitons with more susy (N = 2 for the kink, N = 4 for the monopole) or less susy (N = 1 for the vortex). In addition, discussions have