Consider randomly scattered radio transceivers in ℝd , each of which can transmit signals to all transceivers in a given randomly chosen region about itself. If a signal is retransmitted by every transceiver that receives it, under what circumstances will a signal propagate to a large distance from its starting point? Put more formally, place points {x i } in ℝd  according to a Poisson process with intensity 1. Then, independently for each x i , choose a bounded region A x i  from some fixed distribution and let  be the random directed graph with vertex set
 be the random directed graph with vertex set  whenever x j  ∈ x i  + A x i . We show that, for any
 whenever x j  ∈ x i  + A x i . We show that, for any  will almost surely have an infinite directed path, provided the expected number of transceivers that can receive a signal directly from x i  is at least 1 + η, and the regions x i  + A x i  do not overlap too much (in a sense that we shall make precise). One example where these conditions hold, and so gives rise to percolation, is in ℝd , with each A x i  a ball of volume 1 + η centred at x i , where η → 0 as d → ∞. Another example is in two dimensions, where the A x i  are sectors of angle ε γ and area 1 + η, uniformly randomly oriented within a fixed angle (1 + ε)θ. In this case we can let η → 0 as ε → 0 and still obtain percolation. The result is already known for the annulus, i.e. that the critical area tends to 1 as the ratio of the radii tends to 1, while it is known to be false for the square (l∞) annulus. Our results show that it does however hold for the randomly oriented square annulus.
 will almost surely have an infinite directed path, provided the expected number of transceivers that can receive a signal directly from x i  is at least 1 + η, and the regions x i  + A x i  do not overlap too much (in a sense that we shall make precise). One example where these conditions hold, and so gives rise to percolation, is in ℝd , with each A x i  a ball of volume 1 + η centred at x i , where η → 0 as d → ∞. Another example is in two dimensions, where the A x i  are sectors of angle ε γ and area 1 + η, uniformly randomly oriented within a fixed angle (1 + ε)θ. In this case we can let η → 0 as ε → 0 and still obtain percolation. The result is already known for the annulus, i.e. that the critical area tends to 1 as the ratio of the radii tends to 1, while it is known to be false for the square (l∞) annulus. Our results show that it does however hold for the randomly oriented square annulus.