We consider the tracer diffusion Drr that arises from the run-and-tumble motion of low Reynolds number swimmers, such as bacteria. Assuming a dilute suspension, where the bacteria move in uncorrelated runs of length λ, we obtain an exact expression for Drr for dipolar swimmers in three dimensions, hence explaining the surprising result that this is independent of λ. We compare Drr to the contribution to tracer diffusion from entrainment.As microswimmers, such as bacteria, algae or active colloids, move they produce long-range velocity fields which stir the surrounding fluid. As a result particles and biofilaments suspended in the fluid diffuse more quickly, thus helping to ensure an enhanced nutrient supply. Following the early studies of mixing in concentrated microswimmer suspensions [1][2][3], recent experiments have demonstrated enhanced diffusion in dilute suspensions of Chlamydomonas reinhardtii, Escherichia coli and selfpropelled particles [4][5][6][7][8]. Simulations have found similar behaviour [9][10][11] and microfluidic devices exploiting the enhanced transport due to motile organisms have been suggested [12,13]. However, theoretical description of fluctuations and mixing in active systems remains a challenge even for very dilute suspensions of microswimmers. The statistics of fluid velocity fluctuations was studied in [14][15][16]. As the tracer displacements at short times are proportional to fluid velocities, these results characterise the short-time statistics of tracer displacements. In particular, the fluid velocity fluctuations turn out, generically, non-Gaussian. Features of the long-time tracer displacement statistics remain unknown.The Reynolds number associated with bacterial swimming is ∼ 10 −4 − 10 −6 . Therefore the flow fields that result from the motion obey the Stokes equations and the far velocity field can be described by a multipole expansion. The leading order term in this expansion, the Stokeslet (or Oseen tensor), which decays with distance ∼ r −1 , is the flow field resulting from a point force acting on the fluid. However biological swimmers, which are usually sufficiently small that gravity can be neglected, move autonomously and therefore have no resultant force or torque acting upon them. Hence the Stokeslet term is zero and the flow field produced by the microswimmers contains only higher order multipoles, for example dipolar contributions, ∼ 1/r 2 , and quadrupolar terms, ∼ 1/r 3 .The absence of the Stokeslet term has important repercussions for the way in which tracer particles are advected by swimmers. The angular dependences of the dipolar velocity field -shown in Fig. 1 -and of higher order multipoles of the flow field lead to loop-like tracer trajectories. For a distant swimmer, moving along an infinite * mitya.pushkin@physics.ox.ac.uk straight trajectory these loops are closed.The paths of bacteria or active colloids are, however, far from infinite straight lines. For example, periodic tumbling (abrupt and substantial changes in direction) is a well established mec...