2020
DOI: 10.1109/access.2020.3027813
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High Gain and Low-Profile Stacked Magneto-Electric Dipole Antenna for Phased Array Beamforming

Abstract: A high gain stacked antenna based on a planar magneto-electric dipole structure is proposed. The main radiator is configured by a probe-fed patch with a symmetrically arranged pair of dipole radiation elements. Further, an additional air-gapped radiator with multiple patch elements is integrated for gain enhancement. Since both the main and stacked radiators are planar structures, the overall volume can remain low-profile regardless of the airgap. To verify the performance of the proposed structure, a single m… Show more

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Cited by 12 publications
(6 citation statements)
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“…Notably, the implementation of a co-simulation between the basic ME dipole and its front-feeding circuit necessitates an equivalent circuit model of the antenna. Thus far, many equivalent circuit models have been proposed for this kind of antenna [20][21][22][23]. However, these models failed to reveal the real impedance characteristics of the antenna.…”
Section: Introductionmentioning
confidence: 99%
“…Notably, the implementation of a co-simulation between the basic ME dipole and its front-feeding circuit necessitates an equivalent circuit model of the antenna. Thus far, many equivalent circuit models have been proposed for this kind of antenna [20][21][22][23]. However, these models failed to reveal the real impedance characteristics of the antenna.…”
Section: Introductionmentioning
confidence: 99%
“…But, the metal cavity and high profile makes structure bulky. A low‐profile planar ME antenna loaded by metasurface with a thickness of 0.14 λ 0 proposed in [13] provides 5.2% of bandwidth and maximum gain of 9.6 dBi. A proximity coupled wideband printed ME dipole antenna with 0.19 λ 0 profile shows 54% bandwidth and maximum gain of 9.2 dBi [14].…”
Section: Introductionmentioning
confidence: 99%
“…Several methods have been proposed in the literature for enhancing the performance of planar antennas in terms of gain and directivity, some of which include: (i) arranging planar antennas in an array configuration [32], [33], (ii) loading a reflector layer [34], [35], (iii) utilization of shorting pins to optimize the impedance matching of the planar antenna [36], [37], (iv) employing high permittivity substrates [38], [39], (v) altering the basic shape of the antenna [40], [41], (vi) utilizing multiple substrates [42], [43], (vii) loading artificial materials such as Frequency Selective Surface (FSS) [44][46], Electromagnetic Band-Gap (EBG) [47], [48], Metasurfaces [49], [50], or Artificial Magnetic Conductor (AMC) [51], [52]. However, most of these approaches have drawbacks, such as bulky structures, they are complex and often difficult to fabricate, require complicated power distribution, exhibit narrow bandwidth, etc.…”
Section: Introductionmentioning
confidence: 99%