hologram (CGH) algorithms, such as the algorithms of Gerchberg-Saxton (GS), [14] Yang-Gu, [15] Fienup, [16] and Simulated Annealing. [17][18][19] Diffractive optical elements (DOEs) are a common application of CGH. In particular, DOEs consisting of square phase elements (i.e., pixels) are the easiest to design and fabricate. Each of these elements is a structure with a discrete height or refractive index designed to locally modulate the phase of the transmitted light. When combined, DOEs with diffraction efficiencies as high as 80% can be routinely achieved. [20] DOEs inevitably suffer from the zero order spot that appears as a bright spot in the middle of the projected image. The projected image corresponds to the intensity distribution in the Fourier plane, which is obtained by Fourier transform (FT) of the modified wavefront immediately after the hologram plane. Hence, the zero order spot is also referred to as the DC noise. This bright spot is exacerbated by fabrication imperfections and illumination beyond the extent of the DOE. [20][21][22] For instance, a commercialized liquid crystal spatial light modulator (SLM) with a filling fact or of ≈90% would result in a zero order spot due to light that passes through the dead regions. [23] Transparent dielectric structures fabricated by etching and polymer structure made by lithography would possess defects in the surface topography [11,24] that lead to the zero order spot. Furthermore, the inhomogeneity and dispersive optical property of the phase element materials can impede the performance of DOEs. [25] Ineluctably, a bright zero order spot appears in the center of the Fourier plane, [22,25] Diffractive optical elements (DOEs) provide a compact and energy-efficient solution to project arbitrary grayscale images onto a distant screen. Unfortunately, they invariably suffer from the zero order spot, which is caused mainly by undiffracted light that travels along the optical axis of an illuminating laser beam. To produce projected images without the bright spot, one can either shift the intended projection off-axis or block the zero order. However, images projected by these methods are occluded by the dark fringes of the diffraction pattern ("shadowing" effect) or increase the complexity of the optical setup. Here, a new type of DOE is introduced with blazed facets to shift the laser power into the off-axis direction. By adding blazed facets onto each phase element of a computer-generated hologram, far-field projections that are free of both the zero order spot and shadowing effects are produced while maintaining a diffraction efficiency as high as 86%. The blazed facets are fabricated by 3D direct laser writing, which enables continuous phase modulation within a single pixel. This concept of sub-pixel level modification of diffractive optical elements can be extended to other applications requiring precise wavefront shaping or detection, such as 3D displays, mixed-reality technology, and optical analog computing.