We study the Cauchy problem on the real line for the nonlocal Fisher-KPP equation in one spatial dimension, \begin{equation*} u_t = D u_{xx} + u(1-\phi *u), \end{equation*}
\begin{equation*} u_t = D u_{xx} + u(1-\phi *u), \end{equation*} $\phi *u$ is a spatial convolution with the top hat kernel,
$\phi *u$ is a spatial convolution with the top hat kernel,  $\phi (y) \equiv H\left (\frac{1}{4}-y^2\right )$. After observing that the problem is globally well-posed, we demonstrate that positive, spatially periodic solutions bifurcate from the spatially uniform steady state solution
$\phi (y) \equiv H\left (\frac{1}{4}-y^2\right )$. After observing that the problem is globally well-posed, we demonstrate that positive, spatially periodic solutions bifurcate from the spatially uniform steady state solution  $u=1$ as the diffusivity,
$u=1$ as the diffusivity,  $D$, decreases through
$D$, decreases through  $\Delta _1 \approx 0.00297$ (the exact value is determined in Section 3). We explicitly construct these spatially periodic solutions as uniformly valid asymptotic approximations for
$\Delta _1 \approx 0.00297$ (the exact value is determined in Section 3). We explicitly construct these spatially periodic solutions as uniformly valid asymptotic approximations for  $D \ll 1$, over one wavelength, via the method of matched asymptotic expansions. These consist, at leading order, of regularly spaced, compactly supported regions with width of
$D \ll 1$, over one wavelength, via the method of matched asymptotic expansions. These consist, at leading order, of regularly spaced, compactly supported regions with width of  $O(1)$ where
$O(1)$ where  $u=O(1)$, separated by regions where
$u=O(1)$, separated by regions where  $u$ is exponentially small at leading order as
$u$ is exponentially small at leading order as  $D \to 0^+$. From numerical solutions, we find that for
$D \to 0^+$. From numerical solutions, we find that for  $D \geq \Delta _1$, permanent form travelling waves, with minimum wavespeed,
$D \geq \Delta _1$, permanent form travelling waves, with minimum wavespeed,  $2 \sqrt{D}$, are generated, whilst for
$2 \sqrt{D}$, are generated, whilst for  $0 \lt D \lt \Delta _1$, the wavefronts generated separate the regions where
$0 \lt D \lt \Delta _1$, the wavefronts generated separate the regions where  $u=0$ from a region where a steady periodic solution is created via a distinct periodic shedding mechanism acting immediately to the rear of the advancing front, with this mechanism becoming more pronounced with decreasing
$u=0$ from a region where a steady periodic solution is created via a distinct periodic shedding mechanism acting immediately to the rear of the advancing front, with this mechanism becoming more pronounced with decreasing  $D$. The structure of these transitional travelling wave forms is examined in some detail.
$D$. The structure of these transitional travelling wave forms is examined in some detail.