We consider a quantum dot coupled to a topological superconductor and two normal leads and study transport properties of the system. Using Keldysh path-integral approach, we study current fluctuations (shot noise) within the low-energy effective theory. We argue that the combination of the tunneling conductance and the shot noise through a quantum dot allows one to distinguish between the topological (Majorana) and non-topological (e.g., Kondo) origin of the zero-bias conduction peak. Specifically, we show that, while the tunneling conductance might exhibit zero-bias anomaly due to Majorana or Kondo physics, the shot noise is qualitatively different in the presence of Majorana zero modes.PACS numbers: 73.21. Hb, 71.10.Pm, 74.78.Fk, 72.70.+m Introduction. The search for topological superconductors hosting non-Abelian quasiparticles (defects binding Majorana zero modes) has become an active and exciting pursuit in condensed matter physics [1][2][3]. There has been enormous theoretical and experimental activity in this direction recently [4] fueled, in part, by the potential application of topological superconductors for the faulttolerant topological quantum computation schemes [5]. A large number of theoretical proposals for engineering topological superconductors in the laboratory has been put forward [6][7][8][9][10][11][12][13][14][15], and there has been a significant amount of experimental activity in this area recently [16][17][18][19][20][21][22][23][24][25]. One of the simplest ways to detect the presence of Majorana zero modes (MZMs) in topological superconductors (TSC) is tunneling spectroscopy. Indeed, the presence of MZMs leads to a quantized zero-bias conductance G = 2e 2 /h [26-33]. The pioneering Majorana experiment based on a semiconductor/superconductor heterostructure proposal [10,11] was performed in Delft [16] where the observation of zero-bias peak in a finite magnetic field was reported, consistent with the theoretical predictions [31]. However, other effects might also lead to the zero-bias anomaly which spurred the debate [34][35][36][37][38][39][40][41] as to the precise origin of the (un-quantized) zerobias conduction peak observed in recent tunneling experiments [16][17][18][19][20][21]. Therefore, additional experiments testing other properties on MZMs [17,36,37,[42][43][44][45][46][47][48][49][50][51][52][53][54] are necessary in order to reach a consensus.