Abstract
The principles of formation of antennas of diffraction radiation with flat surface in the millimeter wave radio band are considered. Such kinds of antennas are based on the effect of the conversion of volumetric electromagnetic waves into surface waves of a dielectric waveguide in an open electrodynamic structure. A brief description of the theoretical basis for the calculations and examples of the technical implementation of flat (2D) antennas of diffraction radiation in the W-band and Ka-band are presented; their parameters and areas of possible use are discussed. In the <i>E</i>-plane angle-to-frequency dependence of beam position is realized with coefficient near 0,9/1% of frequency change. That makes it possible effective control of beam position in space (beam scanning along 1, or even along 2 axes). There was estimated that total active loss in such kind antennas is related to dielectric losses in the material of planar dielectric waveguide and to active losses at the elements of internal waveguide transitions in the ratio near (2: 1). Losses of first kind may be reduced due to implementation of novel dielectric materials providing the smallest dielectric loss (near as for the PTFE material) and appropriate mechanical rigidity at the same time. Active losses of the second kind may be reduced due to implementation of transitions on the base of super-size waveguides.
Highlights
One well-studied and widely used class of antennas related to leaky-wave antennas of various types are described in references [1,2,3,4,5]
In a number of publications such kind of electrodynamic structures were named Antennas of Diffraction Radiation (ADR), which some researchers still consider as a sub-class of leaky-wave antennas, and some distinguish this as a separate class of antennas [6, 7]
Without going into details of terminology, it may be noted that the main difference of ADR is in spatial separation of the dielectric waveguide and diffraction grating in the combined electrodynamic structure with their interaction due to appearance of external surface waves of the dielectric waveguide, which have specific properties affecting characteristics of the antenna
Summary
One well-studied and widely used class of antennas related to leaky-wave antennas of various types are described in references [1,2,3,4,5]. At the end of the 1970’s, using the technique of leaky wave antennas, a separate subclass of electrodynamic structures with specific characteristics had appeared They consisted of open electrodynamic structures based on a dielectric waveguide and a diffraction grating spatially spaced, but interconnected by an electromagnetic field. These kinds of emitters are included in the theory and techniques of Antennas of Diffraction Radiation (ADR) During research in this technical area different types of ADR in MM and Sub-MM wave bands were developed on the basis of linear (one-dimensional) and planar (two-dimensional) "open" electromagnetic structures, and their characteristics were described in [7, 12,13,14]. This transition may be formed according to different schemes of the horn, horn-lens, or horn-parabolic antenna with the standard operation mode (i.e. single-mode field structure), or on the basis of a super-dimensional waveguide transition with a multimode structure of the electromagnetic field, including E-type waveguide angular turns of 90 or 180 degrees, which allow optimized dimensions of the entire structure
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More From: American Journal of Electromagnetics and Applications
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