диафрагмированные волноводные фильтры / cebec00e-3d53-4cc6-8501-1eefe793b975
.pdfThis article has been accepted for inclusion in a future issue of this journal. Content is final as presented, with the exception of pagination.
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FIGURE 18. The measured normalized (a) E-plane (xy) coand cross-polar and (b) H-plane (xz) copolar radiation pattern of narrow-band antenna configuration E.
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FIGURE 19. The simulated and measured S11 and maximum realized gain (xy plane) of narrow-band antenna configuration F.
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FIGURE 20. The simulated and measured S11 and maximum realized gain (xy plane) of narrow-band antenna configuration G.
both beneath the substrate and on the multilayered superstrate in the ARMA with shorting copper strips, two different resonances are excited in this configuration, which, in turn, provides a nar- row-band response around each SRR’s resonance frequency. The plots in Figure 20 confirm narrow-band functionality at 6.66 GHz and 7.69 GHz, with a peak measured gain of 3.02 dBi and 1.98 dBi around each SRR pair’s resonance frequency. The simulated efficiency for narrow-band configurations E and F is 86% at 6.58 GHZ and 73% at 7.31 GHz, respectively, and for configuration G, it is 84% and 72% at 6.52 GHz and 7.51 GHz, respectively. The antenna’s measured radiation pattern, shown in Figure 21, indicates a monopole-like omnidirectional character.
Simulated contour plots of the Poynting vector for configurations E, F, and G are shown in Figure 22, which indicates an exactly complementary response to that of notched UWB configurations B, C, and D, respectively, reconfirming the narrow-band antenna response. Antenna configurations E, F, and G are excited at 6.58 GHz, 7.31 GHz, and 6.52 GHz/7.51 GHz, respectively, because of the narrow bandpass response of the SRRand copper-strip-loaded CPW line. We can observe from the plots in Figure 22(a)–(c), all of which indicate nar- row-band excitation of the antenna (configurations E, F, and G), that the distance from the antenna’s feed port to the position of filtering action exactly matches the position of the respective SRR pair and copper strips (on the other side) on the CPW.
CONCLUSIONS
In this article, we presented a new design concept for a multifunctional antenna providing frequency-notched UWB operation and multiple narrowband configurations. We validated the design concept using an electromagnetic solver, circuit simulation, and practical measurements. The proposed technique of achieving frequency notches and narrow-band operation at the same frequency using multilayered
12 |
a p r i l 2 0 1 8 |
IEEE Antennas & PropAgation Magazine |
This article has been accepted for inclusion in a future issue of this journal. Content is final as presented, with the exception of pagination.
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electronic switches with the proper bias |
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arrangement to ensure radio frequency |
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and dc isolation. The proposed design |
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concept can be successfully employed |
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nas required for CR and MIMO appli- |
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cations. |
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AUTHOR INFORMATION |
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Latheef A. Shaik (latheef.a.shaik@ |
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ieee.org) is currently working toward his |
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Ph.D. degree in the Department of Avi- |
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onics, Indian Institute of Space Science |
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and Technology, Thiruvananthapuram. |
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6.66 GHz, Copolar |
7.69 GHz, Copolar |
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6.66 GHz, Cross-Polar |
7.69 GHz, Cross-Polar |
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His research interest are ultrawide-band |
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antennas, reconfigurable antennas, and |
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FIGURE 21. The measured normalized (a) E-plane (xy) plane coand cross-polar and |
dielectric resonator antennas. He is a |
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(b) H-plane (xz) copolar radiation pattern of narrow-band antenna configuration G. |
Student Member of the IEEE. |
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Chinmoy Saha (csaha@ieee.org) is |
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an associate professor in the Depart- |
SRR configurations is unique and compact. Superstrate load- |
ment of Avionics, Indian Institute of Space Science and Technol- |
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ing on the feed section of the antenna to accommodate one |
ogy, Thiruvananthapuram. His research interests include micro- |
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extra pair of SRRs also helps in reducing the antenna footprint. |
wave circuits, engineered materials, metamaterial-inspired |
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Notch frequencies can be tailored by properly choosing the SRR |
antennas and circuits, dielectric resonator antennas, and anten- |
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dimensions beneath the ARMA and/or the SRRs printed above |
nas for space and terahertz applications. He is a Senior Member |
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the superstrate and the latter’s dielectric constant. |
of the IEEE. |
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The practical implementation of the complementary response |
Yahia M.M. Antar (antar-y@rmc.ca) is a professor in the |
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between narrow-band and wide-band frequency-notched |
Department of Electrical and Computer Engineering, Royal |
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functionality of the same antenna (configuration A) requires |
Military College of Canada, Kingston, Ontario. He has authored |
Frequency (GHz)
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FIGURE 22. Three simulated contour plots of Poynting vectors of the propagating electromagnetic energy through the longitudinal dimension of one of the slots as a function of frequency: (a) and (b) configurations E and F, indicating energy propagation at a single frequency, and (c) configuration G, indicating energy propagation at dual frequencies. Narrow-band frequencies are contributed by the corresponding SRR and copper strip.
IEEE Antennas & PropAgation Magazine |
a p r i l 2 0 1 8 |
13 |
This article has been accepted for inclusion in a future issue of this journal. Content is final as presented, with the exception of pagination.
or coauthored more than 200 journal papers, numerous book chapters, and approximately 400 refereed conference papers. He is a Life Fellow of the IEEE.
Jawad Y. Siddiqui (jysiddiqui@ieee.org) is an associate professor in the Department of Radio Physics and Electronics, University of Calcutta, India. His research areas include ultrawideband antennas, frequency reconfigurable antennas, tapered slot antennas, antennas for cognitive radio applications, and ultrawideband radar systems. He is a Senior Member of the IEEE.
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[14]J. Y. Siddiqui, C. Saha, and Y. M. M. Antar, “Compact SRR loaded UWB circular monopole antenna with frequency notch characteristics,” IEEE Trans. Antennas Propag., vol. 62, no. 8, pp. 4015–4020, 2014.
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14 |
a p r i l 2 0 1 8 |
IEEE Antennas & PropAgation Magazine |