A substrate-integrated waveguide (SIW) broadband phase shifter is presented and studied. The phase shift mechanism is based on the synthesis of an artificial dielectric slab using an array of metallic rods in the middle of a SIW. This technique enables a large phase shift within a compact size and enhances the density of integration. As an example, 45°and 90°phase shifters are designed and showcased on a single-layer substrate at a centre frequency of 26 GHz. The amplitude imbalance between the two paths is also avoided while the phase error is less than 5°over a frequency band of 20-32 GHz or around 46% relative bandwidth. The measured return loss is found to be better than 12 dB over the whole frequency band.Introduction: Phase shifters in fixed and variable categories are extremely desired components [1,2]. They are used in a wide variety of applications including wireless communication, radar, measurement and instrumentation systems, as well as antenna array feed and beamforming networks. The use of substrate-integrated waveguide (SIW) technology allows the development of a compact circuit with low radiation loss at millimetre-wave frequencies. Several SIW phase shifters have been proposed and demonstrated [3][4][5].In [3], the phase shifting was realised by means of unequal length, unequal width transmission lines. A differential phase shift of 45 ± 0.4°was achieved together with a reflection coefficient of less than −20 dB over 31-40 GHz (25%) and an insertion loss of <0.7 dB. On the other hand, a SIW phase shifter was developed by H-plane stubs loading in [4] to cover the V-band, with a flat phase difference of 90°over 16% of the frequency band. In such two cases, the main and reference lines have different lengths that may complicate the integration of the phase shifter in a whole network.In [5], the phase-shift mechanism was studied on the basis of the synthesis of a low dielectric slab in the middle of a SIW using an array of air holes (air-field slab). The number of holes, their diameter and their spacing can be adjusted to yield the required phase shift. An experimental validation in the Ka band shows excellent results from 30 to 40 GHz.The last design solution shows a restricted flexibility; in fact, the slab has one possible permittivity (air-field). To achieve a greater phase shifting, unit cells should be cascaded to generate an additive phase shift. Of course, the total size as well as the insertion loss would be increased. The phase shifter using a lower permittivity slab requires a larger dimension compared with its high-permittivity counterpart. It is rather complicated to integrate slabs of different materials in a SIW without altering its shielding propriety. Therefore, the use of an artificial material is proposed in this Letter to allow for permittivity variation.In this Letter, the design platform of the proposed SIW phase shifter is presented and discussed. An array of metallic rods is inserted to increase artificially the dielectric permittivity in the waveguide centre.Parameters are fi...