Slot antenna array synthesis using the infinitesimal dipole model technique: Theory and experiment

Abstract

The present article proposes and validates a new general design methodology that can be used to automatically find proper positions and orientations of waveguidebased radiating slots capable of realizing any given radiation beam profile. The new technique combines basic radiation theory and waveguide propagation theory in an analytical model that permits the prediction of the radiation characteristics of generic slots without the need to perform full-wave numerical solution while completely avoiding using transmission-line models or the slot impedance method. The analytical model is then used to implement a low-cost objective function within a global optimization scheme and subsequently deployed to find optimum positions and orientations of clusters of radiating slots cut into the waveguide surface such that any desired beam pattern can be obtained, leading to very efficient and robust beamforming capability that can be applied to dynamic beamforming in real-time scenarios like MIMO systems. The proposed design method is verified using both full-wave numerical solution and experiment.

Fundamental Spacetime Representations of Quantum Antenna Systems

“…For simplicity, we assume perfect-electric conducting (PEC) antennas where the magnetic field does not contribute to the current Green's function. Another radiating Green's functions similar to G(x, x , t − t ) is needed in expressions such as (A2) in order to obtain the magnetic field B(x, t), which is always present in any radiation problem beside the electric field; see [89][90][91] for more details and applications. The relation (A1) captures the antenna's fundamental Mode A, where a source field E ex (x, t) produces a radiating current via the current Green's function F(x, x , t − t ), which in turn generates the radiated fields E(x, t) and B(x, t) throughout the region exterior to the surface S. To complete the antenna-based wireless communication system, a third Mode C, where a receiving (Rx) antenna, placed at some distance from S, interacts with the radiated field in order to produce an observable receive port current J rx (x) by means of the formula…”

Fundamental Spacetime Representations of Quantum Antenna Systems

“…For simplicity, we assume perfect-electric conducting (PEC) antennas where the magnetic field does not contribute to the current Green's function. Another radiating Green's functions similar to G(x, x , t − t ) is needed in expressions like (82) in order to obtain the magnetic field B(x, t) which is always present in any radiation problem beside the electric field, see [83]- [85] for more details and applications.…”