We show that a planar aperiodic lattice, mimicking the appearance of a sunflower, supports photonic bandgaps for weak dielectric contrast. The pattern's high orientational order and spatially uniform modal pitch yields an isotropic Fourier space. A 2D structure of cylinders ͑⑀ =2͒ in air possesses a wide 21% TM bandgap, versus 5.6% for a sixfold lattice or 14% for a 12-fold fractal tiling. The isotropic gap frequencies imply flat bands, and thus application in nonlinear optics and low threshold lasers, where a reduced group velocity in all directions may be desired. [8]. Intuitively, the ideal Fourier space for 2D band gaps is a circle, i.e., a "Bragg ring." One such pattern with this property is the infinite pinwheel tiling [9]. However, the circular symmetry is not preserved in real (finite) samples.Photonic quasi-crystals are often modeled using periodic "approximants" [8]. In the infinite limit, these approximants recover the properties of the true quasi-periodic parent lattice. PBGs in weakly modulated quasi-crystals are often excluded, even though the approximants may be too small to retain elements of long-range order present in the lattice. In particular, fractal patterns [7,10] may exhibit extremely long-range order owing to their inherent selfsimilarity.In this Letter, we analyze a point set mimicking the head of a sunflower, previously studied in both planar [11] and fiber geometries [12]. Mathematically, this pattern (herein "the sunflower") is a form of Fermat's spiral representing an optimal packing of points evolving about a polar origin. The number of visible spirals, or parastichies, in each direction appear as consecutive numbers in the Fibonacci series, the ratio of which approximates the golden ratio . Formally, an N-point pattern is expressed bywhere ͕n 0:N͖, A is a scaling factor and ⌿ =2 / 2 is the golden angle [13]. This remarkably simple definition contrasts sharply with conventional quasicrystals, typically generated by matching rules, projection, substitution, or multigrids. Figure 1 shows the scanning electron microscopy (SEM) image, Delaunay triangulation, and both calculated and experimental diffraction patterns of a 500 point sunflower fabricated by e-beam lithography. The pattern has a strong modal nearestneighbor pitch a = 2.2 m, derived from Delaunay triangulation [ Fig. 1(b)] of the SEM image ͑r / a = 0.245͒. Expressing the real space density distribution ͑r͒ as a finite sum of plane waves,