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Keywords = mmWave communication

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11 pages, 4261 KiB  
Article
Design of a Half-Mode Substrate-Integrated Waveguide (HMSIW) Multimode Resonator Bandpass Filter Using the Minkowski Fractal for C-Band Applications
by Nitin Muchhal, Abhay Kumar, Nidhi Tewari, Samriti Kalia and Shweta Srivastava
Micromachines 2024, 15(12), 1440; https://doi.org/10.3390/mi15121440 - 28 Nov 2024
Abstract
A substrate-integrated waveguide (SIW) bandpass filter (BPF) with extraordinary selectivity and an adequate upper stopband for C-band Satellite Communication (SATCOM) applications is proposed in this paper. The design comprises comb-shaped slots engraved on a half-mode SIW (HMSIW) that constitute a multimode resonator (MMR). [...] Read more.
A substrate-integrated waveguide (SIW) bandpass filter (BPF) with extraordinary selectivity and an adequate upper stopband for C-band Satellite Communication (SATCOM) applications is proposed in this paper. The design comprises comb-shaped slots engraved on a half-mode SIW (HMSIW) that constitute a multimode resonator (MMR). Its performance is further ameliorated by applying the first and second iterations of the Minkowski fractal curve in the ground plane as a defected ground structure (DGS). The Minkowski fractal has advantages in terms of better bandwidth and miniaturization. The filter is first simulated using the commercial full-wave electromagnetic simulator HFSS v19 and then fabricated on a 0.062′′ (1.6 mm) FR4 with dielectric constant εr = 4.4. The measured results are comparable with the simulated ones and demonstrate that the BPF has a resonant frequency (f0) of 4.75 GHz, a 3 dB bandwidth of 770 MHz (fractional bandwidth of 21.4%), an insertion loss of 1.05 dB, and an out-of-band rejection (in the stopband) of more than 28 dB up to 8 GHz, demonstrating a wide and deep stopband. Using the multimode resonator (MMR) technique, a wide bandwidth has been achieved, and by virtue of using half-mode SIW (HMSIW), the proposed BPF is compact in size. Also, the fractal DGS aids in better stopband performance. Full article
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<p>Half-mode substrate-integrated waveguide with a comb slot.</p>
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<p>Parametric analysis of the transmission response of the comb-shaped curve with respect to edge spacing, S (in mm).</p>
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<p>Simulated S21 response of a comb-slotted MMR filter under weak coupling.</p>
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<p>Mode chart of a comb-slotted MMR filter for different values of L.</p>
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<p>BPF frequency response of the comb-slotted HMSIW.</p>
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<p>First three iterations of the Minkowski fractal curve [<a href="#B22-micromachines-15-01440" class="html-bibr">22</a>].</p>
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<p>First iteration of the Minkowski curve (Li1 = Wi1 = 1.45 mm, Di1 = 1.25 mm).</p>
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<p>BPF using the Minkowski curve’s first iteration level as DGS.</p>
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<p>BPF frequency response based on the Minkowski curve’s first iteration level as the DGS.</p>
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<p>Second iteration of the Minkowski curve (Li2 = Wi2 = 0.45 mm, Di2 = 0.37 mm).</p>
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<p>BPF based on the second iteration level of the Minkowski curve.</p>
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<p>Equivalent circuit of the proposed filter. The element values are Lc = 0.12 nH, Cc = 4.5 pF, Lv = 1.88 nH, Lr = 0.18 nH, and Cr = 7.22 pF.</p>
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<p>BPF frequency response based on the Minkowski curve’s second iteration level as the DGS.</p>
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<p>S parameters of EM simulation and circuit simulation.</p>
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<p>Simulated S21 response of a comb-slotted MMR filter with a DGS under weak coupling.</p>
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<p>Mode chart of a comb-slotted MMR filter with a DGS for various values of L.</p>
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<p>Current distribution in the (<b>a</b>) passband and (<b>b</b>) stopband.</p>
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<p>(<b>a</b>) Upper and (<b>b</b>) bottom views of the fabricated bandpass filter.</p>
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<p>Comparison of the simulated and measured S parameter results.</p>
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<p>Comparison of the simulated and measured group delays.</p>
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43 pages, 4383 KiB  
Review
Integrating UAVs and RISs in Future Wireless Networks: A Review and Tutorial on IoTs and Vehicular Communications
by Mohsen Eskandari and Andrey V. Savkin
Future Internet 2024, 16(12), 433; https://doi.org/10.3390/fi16120433 - 21 Nov 2024
Viewed by 596
Abstract
The rapid evolution of smart cities relies heavily on advancements in wireless communication systems and extensive IoT networks. This paper offers a comprehensive review of the critical role and future potential of integrating unmanned aerial vehicles (UAVs) and reconfigurable intelligent surfaces (RISs) to [...] Read more.
The rapid evolution of smart cities relies heavily on advancements in wireless communication systems and extensive IoT networks. This paper offers a comprehensive review of the critical role and future potential of integrating unmanned aerial vehicles (UAVs) and reconfigurable intelligent surfaces (RISs) to enhance Internet of Vehicles (IoV) systems within beyond-fifth-generation (B5G) and sixth-generation (6G) networks. We explore the combination of quasi-optical millimeter-wave (mmWave) signals with UAV-enabled, RIS-assisted networks and their applications in urban environments. This review covers essential areas such as channel modeling and position-aware beamforming in dynamic networks, including UAVs and IoVs. Moreover, we investigate UAV navigation and control, emphasizing the development of obstacle-free trajectory designs in dense urban areas while meeting kinodynamic and motion constraints. The emerging potential of RIS-equipped UAVs (RISeUAVs) is highlighted, along with their role in supporting IoVs and in mobile edge computing. Optimization techniques, including convex programming methods and machine learning, are explored to tackle complex challenges, with an emphasis on studying computational complexity and feasibility for real-time operations. Additionally, this review highlights the integrated localization and communication strategies to enhance UAV and autonomous ground vehicle operations. This tutorial-style overview offers insights into the technical challenges and innovative solutions of the next-generation wireless networks in smart cities, with a focus on vehicular communications. Finally, future research directions are outlined. Full article
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<p>Organization of the paper based on the taxonomy of the UAV-enabled, RIS-assisted communication into quintuple studied and topics.</p>
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<p>Illustration of direct LoS path and multi-path.</p>
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<p>UAV-enabled, RIS-assisted communication: (<b>a</b>) RISeUAV with a UPA of the RIS aligned in the XY plane facing the ground; (<b>b</b>) UAV-BS as an active aerial (airborne) BS.</p>
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<p>Schematic of RISeUAV-assisted communication for channel modeling: (<b>a</b>) geometry of system in 3D coordinates; (<b>b</b>) UPA of the RIS in XY plane; <math display="inline"><semantics> <mrow> <msup> <mrow> <mi>v</mi> </mrow> <mrow> <mi>R</mi> <mi>U</mi> </mrow> </msup> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msup> <mrow> <mi>u</mi> </mrow> <mrow> <mi>R</mi> <mi>U</mi> </mrow> </msup> </mrow> </semantics></math> denote UAV’s horizontal and vertical linear velocities, respectively; <math display="inline"><semantics> <mrow> <msup> <mrow> <mi>ω</mi> </mrow> <mrow> <mi>R</mi> <mi>U</mi> </mrow> </msup> </mrow> </semantics></math> denotes the UAV’s horizontal rotational velocity and <math display="inline"><semantics> <mrow> <msup> <mrow> <mi>θ</mi> </mrow> <mrow> <mi>R</mi> <mi>U</mi> </mrow> </msup> </mrow> </semantics></math> denotes the UAV heading (angle) with respect to the X-axis. The UAV motion is studied in <a href="#sec4-futureinternet-16-00433" class="html-sec">Section 4</a>.</p>
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<p>Schematic of UAV-enabled, RIS-assisted wireless communication for intelligent vehicles (IVs) in IoVs with mMIMO BSs. Notice that, for the sake of illustration, the sizes of the mMIMO BS and RISeUAV are exaggerated compared with the distances.</p>
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<p>Aerial backhauling through the RISeUAV to UAV-BSs.</p>
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<p>The schematic of the actor-critic deep deterministic policy gradient DRL agent.</p>
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<p>The geometry of the SLAPS for RISeUAV.</p>
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19 pages, 7130 KiB  
Review
Recent Trend of Rate-Splitting Multiple Access-Assisted Integrated Sensing and Communication Systems
by Sukbin Jang, Nahyun Kim, Gayeong Kim and Byungju Lee
Electronics 2024, 13(23), 4579; https://doi.org/10.3390/electronics13234579 - 21 Nov 2024
Viewed by 384
Abstract
In the next-generation communication systems, multiple access (MA) will play a crucial role in achieving high throughput to support future-oriented services. Recently, rate-splitting multiple access (RSMA) has received much attention from both academia and industry due to its ability to flexibly mitigate inter-user [...] Read more.
In the next-generation communication systems, multiple access (MA) will play a crucial role in achieving high throughput to support future-oriented services. Recently, rate-splitting multiple access (RSMA) has received much attention from both academia and industry due to its ability to flexibly mitigate inter-user interference in a broad range of interference regimes. Further, with the growing emphasis on spectrum resource utilization, integrated sensing and communication (ISAC) technology, which improves spectrum efficiency by merging communication and radar signals, is expected to be one of the key candidate technologies for the sixth-generation (6G) wireless networks. In this paper, we first investigate the evolution of existing MA techniques and basic principles of RSMA-assisted ISAC systems. Moreover, to make the future RSMA-assisted ISAC systems, we highlight prime technologies of 6G such as non-terrestrial networks (NTN), reconfigurable intelligent surfaces (RIS), millimeter wave (mmWave) and terahertz (THz) technologies, and vehicular-to-everything (V2X), along with the main technical challenges and potential benefits to pave the way for RSMA-assisted ISAC systems. Full article
(This article belongs to the Special Issue Multi-Scale Communications and Signal Processing)
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<p>Evolution of mobile communication from 1G to 6G.</p>
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<p>Resource allocation for various MA technologies.</p>
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<p>RSMA tranceiver architecture.</p>
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<p>RSMA-assisted ISAC systems.</p>
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<p>RSMA-assisted LEO-ISAC systems.</p>
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<p>RSMA-assisted RIS-ISAC systems.</p>
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<p>RSMA-assisted ISAC systems with hybrid beamforming.</p>
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21 pages, 9459 KiB  
Article
Development and Space Experiment Verification of Annular Liquid Flow Payload for China Space Station
by Jia Wang, Yi Chen, Di Wu, Liang Hu, Zhijun Ye, Li Duan, Xilin Zhao, Yongli Yin and Qi Kang
Symmetry 2024, 16(11), 1530; https://doi.org/10.3390/sym16111530 - 15 Nov 2024
Viewed by 351
Abstract
The annular flow payload is among the first batch of space science experimental projects carried out on the Fluid Physics Rack of the China Space Station. This paper provides a detailed introduction to the development of the payload, ground validation, and in orbit [...] Read more.
The annular flow payload is among the first batch of space science experimental projects carried out on the Fluid Physics Rack of the China Space Station. This paper provides a detailed introduction to the development of the payload, ground validation, and in orbit experiments. The payload, sized 320 mm × 200 mm × 220 mm, includes an annular flow model and supports supply (24 V, 12 V, and 5 V), communication, and data transmission. A multi-functional heating column in the annular flow model was designed, allowing for the column to operate in fixed, rotating, and lifting scenarios. In the first round, 96 sets of space experiments covering volume ratio ranges from 0.45 to 1.06 were carried out. The annular flow liquid surface state, temperature oscillation, and infrared temperature field evolution were obtained. Mode decomposition shows the oscillatory convection of the m = 4 travelling wave, and contains m = 3, m = 6, and m = 8 waves. Full article
(This article belongs to the Section Physics)
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<p>Annular liquid flow model.</p>
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<p>Annular liquid flow payload: (<b>a</b>) payload model diagram; (<b>b</b>) physical diagram of the payload.</p>
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<p>Composition of the annular flow payload system.</p>
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<p>Internal structure of the annular flow payload.</p>
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<p>Central column rotates clockwise in ground experiment. The arrow indicates that the rotation direction of the central column is clockwise. (<b>a</b>) <span class="html-italic">t</span> = <span class="html-italic">τ</span>; (<b>b</b>) <span class="html-italic">t</span> = <span class="html-italic">τ</span> + 1/4 period; (<b>c</b>) <span class="html-italic">t</span> = <span class="html-italic">τ</span> + 1/2 period.</p>
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<p>Central column rising process in ground experiment. The arrow indicates the movement direction of the central column, which is upward. (<b>a</b>) The height of the central column from the bottom of the pool is 3.53 mm; (<b>b</b>) The height of the central column from the bottom of the pool is 4.70 mm; (<b>c</b>) The height of the central column from the bottom of the pool is 5.56 mm.</p>
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<p>Infrared images of HTWs with different wave numbers in ground experiment. (<b>a</b>) HTWs with <span class="html-italic">m</span> = 3, <span class="html-italic">Vr</span> = 0.2, 1.5 cSt, Δ<span class="html-italic">T</span> = <span class="html-italic">T</span><sub>H</sub> − <span class="html-italic">T</span><sub>L</sub> = 36 °C − 12 °C = 24 °C; (<b>b</b>) the corresponding circumferential temperature time evolution of (<b>a</b>); (<b>c</b>) HTWs with <span class="html-italic">m</span> = 4, <span class="html-italic">Vr</span> = 0.15, 1.5 cst, Δ<span class="html-italic">T</span> = <span class="html-italic">T</span><sub>H</sub> − <span class="html-italic">T</span><sub>L</sub> = 30 °C − 10 °C = 20 °C; (<b>d</b>) the corresponding circumferential temperature time evolution of (<b>c</b>); (<b>e</b>) HTWs with m = 5, <span class="html-italic">Vr</span> = 0.15, 1 cst, Δ<span class="html-italic">T</span> = <span class="html-italic">T</span><sub>H</sub> − <span class="html-italic">T</span><sub>L</sub> = 27 °C − 11 °C = 16 °C; (<b>f</b>) the corresponding circumferential temperature time evolution of (<b>e</b>); (<b>g</b>) HTWs with <span class="html-italic">m</span> = 6, <span class="html-italic">Vr</span> = 0.10, 1 cst, Δ<span class="html-italic">T</span> = <span class="html-italic">T</span><sub>H</sub> − <span class="html-italic">T</span><sub>L</sub> = 27 °C − 13 °C = 14 °C; (<b>h</b>) the corresponding circumferential temperature time evolution of (<b>g</b>); (<b>i</b>) disordered waveform, <span class="html-italic">Vr</span> = 0.15, 1 cst, Δ<span class="html-italic">T</span> = <span class="html-italic">T</span><sub>H</sub> − <span class="html-italic">T</span><sub>L</sub> = 60 °C − 15 °C = 45 °C; (<b>j</b>) the corresponding circumferential temperature time evolution of (<b>i</b>).</p>
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<p>Infrared images of HTWs with different wave numbers in ground experiment. (<b>a</b>) HTWs with <span class="html-italic">m</span> = 3, <span class="html-italic">Vr</span> = 0.2, 1.5 cSt, Δ<span class="html-italic">T</span> = <span class="html-italic">T</span><sub>H</sub> − <span class="html-italic">T</span><sub>L</sub> = 36 °C − 12 °C = 24 °C; (<b>b</b>) the corresponding circumferential temperature time evolution of (<b>a</b>); (<b>c</b>) HTWs with <span class="html-italic">m</span> = 4, <span class="html-italic">Vr</span> = 0.15, 1.5 cst, Δ<span class="html-italic">T</span> = <span class="html-italic">T</span><sub>H</sub> − <span class="html-italic">T</span><sub>L</sub> = 30 °C − 10 °C = 20 °C; (<b>d</b>) the corresponding circumferential temperature time evolution of (<b>c</b>); (<b>e</b>) HTWs with m = 5, <span class="html-italic">Vr</span> = 0.15, 1 cst, Δ<span class="html-italic">T</span> = <span class="html-italic">T</span><sub>H</sub> − <span class="html-italic">T</span><sub>L</sub> = 27 °C − 11 °C = 16 °C; (<b>f</b>) the corresponding circumferential temperature time evolution of (<b>e</b>); (<b>g</b>) HTWs with <span class="html-italic">m</span> = 6, <span class="html-italic">Vr</span> = 0.10, 1 cst, Δ<span class="html-italic">T</span> = <span class="html-italic">T</span><sub>H</sub> − <span class="html-italic">T</span><sub>L</sub> = 27 °C − 13 °C = 14 °C; (<b>h</b>) the corresponding circumferential temperature time evolution of (<b>g</b>); (<b>i</b>) disordered waveform, <span class="html-italic">Vr</span> = 0.15, 1 cst, Δ<span class="html-italic">T</span> = <span class="html-italic">T</span><sub>H</sub> − <span class="html-italic">T</span><sub>L</sub> = 60 °C − 15 °C = 45 °C; (<b>j</b>) the corresponding circumferential temperature time evolution of (<b>i</b>).</p>
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<p>Quasi-equilibrium state, hydrothermal wave with <span class="html-italic">m</span> = 6, <span class="html-italic">Vr</span> = 0.15, 1 cst, Δ<span class="html-italic">T</span> = <span class="html-italic">T</span><sub>H</sub> − <span class="html-italic">T</span><sub>L</sub> = 26 °C − 11 °C = 15 °C. The time interval from (<b>a</b>) to (<b>d</b>) is 1 s. (<b>a</b>) <span class="html-italic">t</span> = <span class="html-italic">τ</span>; (<b>b</b>) <span class="html-italic">t</span> = <span class="html-italic">τ</span> + 1 s; (<b>c</b>) <span class="html-italic">t</span> = <span class="html-italic">τ</span> + 2 s; (<b>d</b>) <span class="html-italic">t</span> = <span class="html-italic">τ</span> + 3 s. The red area <span class="html-italic">R</span>0 is an identification area made for facilitating the display of the rotation of the central column.</p>
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<p>Installation of the annular flow payload in the fluid cabinet (red area).</p>
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<p>On-orbit experiment process of the annular flow payload.</p>
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<p>Annular liquid flow in space. (<b>a</b>) Fixed central column: on the free surface, under the action of surface tension, the liquid flows from the center to the side wall. Following the conservation of mass, the liquid at the bottom flows back to the central column from the side wall. (<b>b</b>) Central column lifting: it can be lifted from the bottom to 15 mm. (<b>c</b>) Central column rotation: it can move clockwise or counterclockwise.</p>
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<p>Temporal evolution of temperature (circumferential): (<b>a</b>) the infrared image after modal decomposition, <span class="html-italic">Vr</span> = 1.05, 2 cSt, Δ<span class="html-italic">T</span> = <span class="html-italic">T</span><sub>H</sub> − <span class="html-italic">T</span><sub>L</sub> = 44 °C − 24 °C = 20 °C; (<b>b</b>) the corresponding circumferential temperature–time evolution.</p>
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<p>Modal decomposition of annular flow data (arranged according to the energy of HTWs), <span class="html-italic">Vr</span> = 1.0, 2 cSt, Δ<span class="html-italic">T</span> = <span class="html-italic">T</span><sub>H</sub> − <span class="html-italic">T</span><sub>L</sub> = 43 °C − 23 °C = 20 °C. (<b>a</b>) Infrared disturbance image after subtracting the average value, <span class="html-italic">m</span> = 4; (<b>b</b>) infrared disturbance images during heating and cooling; (<b>c</b>) <span class="html-italic">m</span> = 4, traveling wave, clockwise; (<b>d</b>) <span class="html-italic">m</span> = 8, harmonic wave; (<b>e</b>) <span class="html-italic">m</span> = 6, harmonic wave; (<b>f</b>) <span class="html-italic">m</span> = 8, harmonic wave; (<b>g</b>) <span class="html-italic">m</span> = 3, harmonic wave; (<b>h</b>) <span class="html-italic">m</span> = 8, harmonic wave.</p>
Full article ">Figure 13 Cont.
<p>Modal decomposition of annular flow data (arranged according to the energy of HTWs), <span class="html-italic">Vr</span> = 1.0, 2 cSt, Δ<span class="html-italic">T</span> = <span class="html-italic">T</span><sub>H</sub> − <span class="html-italic">T</span><sub>L</sub> = 43 °C − 23 °C = 20 °C. (<b>a</b>) Infrared disturbance image after subtracting the average value, <span class="html-italic">m</span> = 4; (<b>b</b>) infrared disturbance images during heating and cooling; (<b>c</b>) <span class="html-italic">m</span> = 4, traveling wave, clockwise; (<b>d</b>) <span class="html-italic">m</span> = 8, harmonic wave; (<b>e</b>) <span class="html-italic">m</span> = 6, harmonic wave; (<b>f</b>) <span class="html-italic">m</span> = 8, harmonic wave; (<b>g</b>) <span class="html-italic">m</span> = 3, harmonic wave; (<b>h</b>) <span class="html-italic">m</span> = 8, harmonic wave.</p>
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<p>Annular flow space scientific data: (<b>a</b>) temperature data collected by thermocouples, and the arrow indicates the critical oscillation point; (<b>b</b>) frequency analysis of temperature data collected by thermocouples, the main frequency <span class="html-italic">f</span><sub>0</sub> = 0.30 Hz; (<b>c</b>) original infrared image; (<b>d</b>) processed infrared image.</p>
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<p>Chaotic attractor: (<b>a</b>) position of selected point, <span class="html-italic">P</span><sub>a</sub>; (<b>b</b>) time histories of the temperature oscillations; (<b>c</b>) phase space reconstructions; (<b>d</b>) <span class="html-italic">λ</span> (Lyapunov exponent) calculation by the small data method. <span class="html-italic">T</span> (<span class="html-italic">τ</span>) is the temperature at time <span class="html-italic">τ</span>.</p>
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16 pages, 6867 KiB  
Article
Reconstructing Signals in Millimeter Wave Channels Using Bayesian-Based Fading Models
by Claudio Bastos Silva, Pedro E. Pompilio, Theoma S. Otobo and Horacio Tertuliano Filho
Electronics 2024, 13(22), 4406; https://doi.org/10.3390/electronics13224406 - 11 Nov 2024
Viewed by 469
Abstract
Fading in communication channels presents eminently stochastic characteristics and is a significant challenge, especially at millimeter wave (mmW) frequencies, where the need for lines of sight and the high attenuation of obstacles complicate transmission. This article presents a model based on Bayesian fundamentals [...] Read more.
Fading in communication channels presents eminently stochastic characteristics and is a significant challenge, especially at millimeter wave (mmW) frequencies, where the need for lines of sight and the high attenuation of obstacles complicate transmission. This article presents a model based on Bayesian fundamentals intended to improve the description and simulation of stochastic fading effects in these channels. It also includes the use of signal processing techniques to simulate and reconstruct the received signal, simulating the communication channel with an FIR filter. The results obtained by simulating the model show its ability to efficiently capture rapid and profound variations in the signal, typical of those that occur in urban and suburban environments and transmissions in the mmW spectrum. It also provides greater uniformity in signal reconstruction compared to the traditional models that are in use. Using Bayesian fundamentals, which allow dynamic adaptation to change in channel behavior, can improve the efficiency and reliability of networks, especially modern smart networks. Compared to traditional models, the proposed model offers improved signal reconstruction and fading mitigation accuracy, with prospects for future integration in smart communication systems. The better capacity in signal reconstruction presents itself as a differentiator of the model, suggesting greater precision in data transmission. Full article
(This article belongs to the Special Issue Advances in Signal Processing for Wireless Communications)
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<p>(<b>a</b>) Noise distribution histogram and (<b>b</b>) QQplot for normal distribution.</p>
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<p><math display="inline"><semantics> <mi mathvariant="script">L</mi> </semantics></math> distribution’s behavior as a function of the variation in <span class="html-italic">Y</span>.</p>
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<p>Pure sinusoidal and received signal with noise. (<b>a</b>) <math display="inline"><semantics> <mi mathvariant="script">L</mi> </semantics></math> model; (<b>b</b>) Nakagami.</p>
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<p>Compared dispersion of amplitude distribution.</p>
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<p>Channel unitary impulse response simulated for a sample in the period.</p>
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<p>Reconstructed signal: (<b>a</b>) <math display="inline"><semantics> <mi mathvariant="script">L</mi> </semantics></math> model; (<b>b</b>) Nakagami.</p>
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<p>Comparative PDFs of reconstructed signal noise.</p>
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<p>Comparative fade channel power of reconstructed signals.</p>
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<p>Reconstructed signal for the <math display="inline"><semantics> <mi mathvariant="script">L</mi> </semantics></math> model using (<b>a</b>) traditional reconstruction and (<b>b</b>) particle filter techniques.</p>
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<p>Line plot of reconstructed signal noise power in dB (<math display="inline"><semantics> <mi mathvariant="script">L</mi> </semantics></math> model).</p>
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<p>Power spectral density of reconstructed signal noise (<math display="inline"><semantics> <mi mathvariant="script">L</mi> </semantics></math> model).</p>
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13 pages, 635 KiB  
Article
A Study of Transmission Point Selection for Multi-Connectivity in Multi-Band Wireless Networks
by Eunkyung Kim, Dongwan Kim and Changbeom Choi
Appl. Sci. 2024, 14(22), 10256; https://doi.org/10.3390/app142210256 - 7 Nov 2024
Viewed by 550
Abstract
In 5th generation mobile communication networks, the frequency band of the millimeter band of 30–100 GHz is supported to provide a transmission speed of 20 Gbps or higher. Furthermore, a huge transmission capacity, i.e., up to 1 Tbps, is one of the main [...] Read more.
In 5th generation mobile communication networks, the frequency band of the millimeter band of 30–100 GHz is supported to provide a transmission speed of 20 Gbps or higher. Furthermore, a huge transmission capacity, i.e., up to 1 Tbps, is one of the main requirements for the 6th generation mobile communication networks. In order to meet this requirement, the terahertz band is considered a new service band. Hence, we consider multi-band network environments, serving the sub-6Hz band, mmWave band, and additionally sub-terahertz band. Furthermore, we introduce the transmission point selection criteria with multiple connections for efficient multi-connectivity operation in a multi-band network environment, serving and receiving multiple connections from those bands at the same time. We also propose a point selection algorithm based on the selection criteria, e.g., achievable data rate. The proposed point selection algorithm attains lower computational complexity with a 2-approximation of the optimal solution. Our simulation results, applying the channel environment and beamforming in practical environments defined by 3GPP, show that selecting and serving multiple transmission points regardless of frequency band performs better than services through single-connectivity operation. Full article
(This article belongs to the Special Issue Communication Networks: From Technology, Methods to Applications)
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<p>Examples of multi-band multi-connectivity operation in mobile communication networks: (<b>a</b>) data transmission with a connectivity from single band (e.g., user 1 with FR2, user 2 with FR3, and user 3 with FR1), (<b>b</b>) data transmissions with two connectivities from two bands (e.g., user 4 with FR2 and FR3 and user 5 with FR1 and FR2), and (<b>c</b>) data transmissions with three connectivities from three bands (e.g., user 6 with FR1, FR2, and FR3).</p>
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<p>An example of deployment with TPs (X: TP operating in FR1; O: TP operating in FR2; and □: TP operating in FR3) in UMi-Street Canyon environment, where 4 TPs operating in FR1, 6 TPs operating in FR2, and 8 TPs operating in FR3 are assumed to be deployed at 3m height.</p>
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<p>The average received data rate with different number of users (U = 1, 10, 20, …, 100) in case of that (<b>a</b>) only one connection is allowed for a user (C = 1), (<b>b</b>) two connections are allowed for a user (C = 2), and (<b>c</b>) three connections are allowed for a user (C = 3).</p>
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<p>TP and/or serving beam change rate with different users (U = 1, 10, …, 100) in the case where (<b>a</b>) only one connection is allowed (C = 1), (<b>b</b>) two connections are allowed (C = 2), and (<b>c</b>) three connections are allowed (C = 3).</p>
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17 pages, 5128 KiB  
Article
A Compact Ultra-Wideband Millimeter-Wave Four-Port Multiple-Input Multiple-Output Antenna for 5G Internet of Things Applications
by Ashutosh Sharma, Sanjeev Sharma, Vikas Sharma, Girish Wadhwa and Rajeev Kumar
Sensors 2024, 24(22), 7153; https://doi.org/10.3390/s24227153 - 7 Nov 2024
Viewed by 543
Abstract
This paper presents a compact design for a four-element multiple-input multiple-output (MIMO) antenna for millimeter-wave (mmWave) communications covering the bands of n257/n258/n261. The MIMO design covers the frequency range of 24.25–29.5 GHz, with a wide bandwidth of 5.25 GHz. The element of the [...] Read more.
This paper presents a compact design for a four-element multiple-input multiple-output (MIMO) antenna for millimeter-wave (mmWave) communications covering the bands of n257/n258/n261. The MIMO design covers the frequency range of 24.25–29.5 GHz, with a wide bandwidth of 5.25 GHz. The element of the MIMO antenna structure uses a single circular patch with an inset feed, and, in order to improve the reflection coefficient (S11), a half-disk parasitic patch is positioned on top of the circular patch. Moreover, to fine-tune the antenna’s characteristics, two vertical stubs on the extreme ends of the ground plane are introduced. For this design, a Rogers RT/Duroid 5880 substrate with ultra-thin thickness is used. After the optimization of the design, the four-port MIMO antenna attained a tiny size, with the dimensions 16.2 mm × 16.2 mm × 0.254 mm. In terms of the MIMO parameters, the ECC (Envelop Correlation coefficient) is less than 0.002 and the DG (Diversity Gain) is greater than 9.99 dB in the mentioned band, which are within the tolerance limits. Also, in spite of the very small size and the four-port configuration, the achieved isolation between the neighboring MIMO elements is less than −23.5 dB. Full article
(This article belongs to the Section Internet of Things)
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<p>Design structure of single-element antenna. (<b>a</b>) Single element of MIMO antenna design. (<b>b</b>) Feedline with circular and semi-circular patch.</p>
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<p>Reflection coefficient (S<sub>11</sub>) vs. frequency for single-element antenna.</p>
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<p>Step-wise antenna design.</p>
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<p>Radiating and parasitic patch equivalent circuit.</p>
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<p>E field distribution analysis between radiating and parasitic patch.</p>
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<p>Optimization of S<sub>11</sub> and resonant frequency using (<b>a</b>) R3 and (<b>b</b>) St.</p>
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<p>Optimization of S<sub>11</sub> with (<b>a</b>) W and (<b>b</b>) Sh.</p>
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<p>MIMO antenna design. (<b>a</b>) Top view, (<b>b</b>) modified feedline.</p>
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<p>Fabricated prototype of the proposed antenna. (<b>a</b>) Feed-plane, (<b>b</b>) ground plane.</p>
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<p>Results. (<b>a</b>) Reflection coefficients measured and simulated, (<b>b</b>) simulated isolation, (<b>c</b>) measured isolation, (<b>d</b>) gain vs. frequency plot.</p>
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<p>Results. (<b>a</b>) Reflection coefficients measured and simulated, (<b>b</b>) simulated isolation, (<b>c</b>) measured isolation, (<b>d</b>) gain vs. frequency plot.</p>
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<p>Decoupling due to protruding stubs.</p>
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<p>Radiation characteristics. (<b>a</b>) Antenna-1. (<b>b</b>) Antenna-2. (<b>c</b>) Antenna-3. (<b>d</b>) Antenna-4.</p>
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<p>Radiation characteristics. (<b>a</b>) Antenna-1. (<b>b</b>) Antenna-2. (<b>c</b>) Antenna-3. (<b>d</b>) Antenna-4.</p>
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<p>(<b>a</b>) Envelop Correlation coefficient. (<b>b</b>) Diversity Gain.</p>
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<p>(<b>a</b>) TARC. (<b>b</b>) CCL.</p>
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<p>Surface current for Antenna-1 at 27 GHz. (<b>a</b>) Feed-plane (top view). (<b>b</b>) Ground plane (top view).</p>
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14 pages, 14063 KiB  
Article
High Absorption of Electromagnetic Waves Based on 3D PMMA@Mxene@Co3O4 Composite Microsphere
by Jinghe Guo, Yanxiang Wang, Lanzhou Wang, Bohan Ding, Yongbo Wang, Yue Sun, Shichao Dai, Donglong Wang and Shishuai Bi
Materials 2024, 17(22), 5427; https://doi.org/10.3390/ma17225427 - 6 Nov 2024
Viewed by 415
Abstract
With the increasing demand for effective electromagnetic wave (EMW) absorbers due to the proliferation of electronic devices and 5G communication systems, traditional wave-absorbing materials can no longer meet the current requirements. Thus, this research introduces a three-dimensional (3D) composite material consisting of PMMA@Mxene@Co₃O₄ [...] Read more.
With the increasing demand for effective electromagnetic wave (EMW) absorbers due to the proliferation of electronic devices and 5G communication systems, traditional wave-absorbing materials can no longer meet the current requirements. Thus, this research introduces a three-dimensional (3D) composite material consisting of PMMA@Mxene@Co₃O₄ microspheres, prepared through in situ self-assembly and hydrothermal growth. The strong electrical conductivity of Mxene, combined with the magnetic loss of Co₃O₄, ensures enhanced dielectric–magnetic synergy, leading to excellent EMW absorption. The study investigates the influence of varying Co₃O₄ content on the electromagnetic properties of the composite. Experimental results show that the optimal sample, with a thickness of 2.5 mm, achieves a minimum reflection loss (RLmin) of −52.88 dB at 6.88 GHz and an effective absorption bandwidth (EAB) of 5.28 GHz. This work highlights the potential of 3D PMMA@Mxene@Co₃O₄ composites as high-performance microwave absorbers, providing a promising solution to EMW pollution. The findings offer valuable insights into material design strategies, demonstrate a promising pathway for developing lightweight, high-performance EMW absorbing materials by optimizing impedance matching and utilizing advanced microstructure design techniques. Full article
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<p>Schematic diagram of the preparation process of 3D PMMA@Mxene@Co<sub>3</sub>O<sub>4</sub> composite microspheres.</p>
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<p>SEM images of the (<b>a</b>) PMMA; (<b>b</b>,<b>c</b>) PMMA@MXene; (<b>d</b>) elemental mapping images of PMMA@MXene, TEM and HRTEM images of the (<b>e</b>,<b>f</b>) few-layered MXene; (<b>g</b>,<b>h</b>) PMMA@MXene; and (<b>i</b>) XRD patterns of MAX and MXene.</p>
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<p>(<b>a</b>) XRD patterns of MXene, PMMA and PMMA@Mxene; (<b>b</b>) XRD patterns of 3D PMMA@Mxene@Co<sub>3</sub>O<sub>4</sub> samples.</p>
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<p>SEM images for 3D PMMA@Mxene@Co<sub>3</sub>O<sub>4</sub> samples: (<b>a</b>,<b>d</b>) PMC-1; (<b>b</b>,<b>e</b>) PMC-2; (<b>c</b>,<b>f</b>) PMC-3, TEM and HRTEM images of the (<b>g</b>,<b>h</b>) PMC-2; and (<b>i</b>) elemental mapping images of PMC-2 sample.</p>
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<p>(<b>a</b>,<b>b</b>) Real and imaginary parts of permittivity of the PMMA@MXene, 3D PMMA@MXene@Co<sub>3</sub>O<sub>4</sub>. (<b>c</b>,<b>d</b>) Real and imaginary parts of permeability of the 3D PMMA@MXene@Co<sub>3</sub>O<sub>4</sub> samples.</p>
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<p>3D plots of the frequency dependence and RL curves of (<b>a</b>,<b>b</b>) PMMA@MXene@Co<sub>3</sub>O<sub>4</sub>−1; (<b>c</b>,<b>d</b>) PMMA@MXene@Co<sub>3</sub>O<sub>4</sub>−2; and (<b>e</b>,<b>f</b>) PMMA@MXene@Co<sub>3</sub>O<sub>4</sub>−3 samples.</p>
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<p>(<b>a</b>) Comparison of Rl<sub>min</sub> and EAB of PMMA@Mxene and 3D PMMA@Mxene@Co<sub>3</sub>O<sub>4</sub> samples; (<b>b</b>) RL and EAB of Mxene-based composites [<a href="#B3-materials-17-05427" class="html-bibr">3</a>,<a href="#B7-materials-17-05427" class="html-bibr">7</a>,<a href="#B18-materials-17-05427" class="html-bibr">18</a>,<a href="#B19-materials-17-05427" class="html-bibr">19</a>,<a href="#B25-materials-17-05427" class="html-bibr">25</a>,<a href="#B34-materials-17-05427" class="html-bibr">34</a>,<a href="#B43-materials-17-05427" class="html-bibr">43</a>,<a href="#B44-materials-17-05427" class="html-bibr">44</a>].</p>
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<p>Schematic of electromagnetic wave absorption mechanism of 3D PMMA@Mxene@Co<sub>3</sub>O<sub>4</sub> sample.</p>
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13 pages, 1510 KiB  
Article
A Three-Dimensional Time-Varying Channel Model for THz UAV-Based Dual-Mobility Channels
by Kai Zhang, Fenglei Zhang, Yongjun Li, Xiang Wang, Zhaohui Yang, Yuanhao Liu, Changming Zhang and Xin Li
Entropy 2024, 26(11), 924; https://doi.org/10.3390/e26110924 - 30 Oct 2024
Viewed by 453
Abstract
Unmanned aerial vehicle (UAV) as an aerial base station or relay device is a promising technology to rapidly provide wireless connectivity to ground device. Given UAV’s agility and mobility, ground user’s mobility, a key question is how to analyze and value the performance [...] Read more.
Unmanned aerial vehicle (UAV) as an aerial base station or relay device is a promising technology to rapidly provide wireless connectivity to ground device. Given UAV’s agility and mobility, ground user’s mobility, a key question is how to analyze and value the performance of UAV-based wireless channel in the terahertz (THz) band. In this paper, a three-dimensional (3D) time-varying channel model is proposed for UAV-based dual-mobility wireless channels based on geometric channel model theory in THz band. In this proposed channel model, the small-scale fading (e.g., scattering fading and reflection fading) on rough surfaces of communication environment and the atmospheric molecule absorption attenuations are considered in THz band. Moreover, the statistical properties of the proposed channel model, including path loss, time autocorrelation function (T-ACF) and Doppler power spectrum density (DPSD), have been derived and the impact of several important UAV-related and vehicle-related parameters have been investigated and compared to millimeter wave (mm-wave) band. Furthermore, the correctness of the proposed channel model has been verified via simulation, and some useful observations are provided for the system design of THz UAV-based dual-mobility wireless communication systems. Full article
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<p>Real UAV-based dual-mobility wireless communications scenario in the THz band.</p>
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<p>Different propagation paths between UAV and vehicle in time-varying UAV-based wireless communication system in the THz band: (<b>a</b>) LoS propagation path survival; (<b>b</b>) LoS propagation path death and NLoS propagation path birth.</p>
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<p>The T-ACF with different moving speeds of Tx and Rx for the NLoS path (including reflection and scattering paths).</p>
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<p>The T-ACF with different vertical distance of Tx and Rx for the NLoS path (including reflection and scattering paths).</p>
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<p>The T-ACF with different power ratio of reflection and scattering propagations for the NLoS path (including reflection and scattering paths).</p>
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<p>The T-ACF with different Ricican <span class="html-italic">K</span>-factor.</p>
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<p>Path loss of the MPCs (including LoS, reflection, and scattering paths) with different carrier frequencies.</p>
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<p>The DPSD with different moving times and different paths.</p>
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15 pages, 2743 KiB  
Article
Reducing Successive Interference Cancellation Iterations in Hybrid Beamforming Multiuser Massive Multiple Input Multiple Output Systems Through Grouping Users with Symmetry Channels
by Hashem Khaled Rehab, Eugeniy Rogozhnikov, Kirill Savenko, Semen Mukhamadiev, Yakov Kryukov and Dmitriy Pokamestov
Symmetry 2024, 16(11), 1437; https://doi.org/10.3390/sym16111437 - 29 Oct 2024
Viewed by 1149
Abstract
This paper presents a comprehensive exploration of advanced beamforming techniques tailored for millimeter-wave (mm-Wave) communication systems. In response to the burgeoning demand for higher data rates, coupled with the constraints of power consumption and hardware complexity, this study focuses on developing a hybrid [...] Read more.
This paper presents a comprehensive exploration of advanced beamforming techniques tailored for millimeter-wave (mm-Wave) communication systems. In response to the burgeoning demand for higher data rates, coupled with the constraints of power consumption and hardware complexity, this study focuses on developing a hybrid beamforming framework optimized for downlink scenarios, specifically targeting groups of users based on the approximate symmetry of their channels. The primary innovation of this research lies in leveraging the symmetry of channels among near users to develop a group-based successive interference cancellation (SIC) algorithm. Unlike traditional approaches that address interference on a per-user basis, this algorithm utilizes channel symmetry within clusters of users to reduce computational complexity and improve the efficiency of SIC. By grouping users with symmetrical channel characteristics, the algorithm simplifies the interference management process while maintaining system performance. The proposed system demonstrates notable advantages over existing non-linear algorithms through extensive simulations and performance evaluations, particularly in terms of spectral efficiency and computational complexity. In this study, we further emphasize the importance of balancing spectral efficiency improvements with reduced computational demands, offering a nuanced trade-off that accommodates various operational requirements. The flexible optimization framework provided showcases the system’s adaptability to diverse deployment scenarios and network configurations. Full article
(This article belongs to the Section Engineering and Materials)
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<p>System diagram of a grouped multi-user massive MIMO system with a hybrid beamforming structure.</p>
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<p>Sum spectral efficiency for various hybrid beamforming algorithms with diverse scenario configurations. Figures (<b>a</b>–<b>f</b>) depict scenarios 1–6, respectively.</p>
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<p>Sum spectral efficiency for various hybrid beamforming algorithms with diverse scenario configurations. Figures (<b>a</b>–<b>f</b>) depict scenarios 1–6, respectively.</p>
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<p>Sum SE performance with different number of BS antennas.</p>
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<p>Sum SE performance with perfect and imperfect CSI.</p>
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17 pages, 34163 KiB  
Article
Analysis of 3D Printed Dielectric Resonator Antenna Arrays for Millimeter-Wave 5G Applications
by Siyu Li, Benito Sanz Izquierdo, Steven Gao and Zhijiao Chen
Appl. Sci. 2024, 14(21), 9886; https://doi.org/10.3390/app14219886 - 29 Oct 2024
Viewed by 573
Abstract
This paper explores the potential use of fused deposition modeling (FDM) technology for manufacturing microwave and millimeter-wave dielectric resonator antennas (DRAs) for 5G and beyond communication systems. DRAs operating at microwave and millimeter-wave (mmWave) frequency bands were simulated, fabricated, and analyzed in terms [...] Read more.
This paper explores the potential use of fused deposition modeling (FDM) technology for manufacturing microwave and millimeter-wave dielectric resonator antennas (DRAs) for 5G and beyond communication systems. DRAs operating at microwave and millimeter-wave (mmWave) frequency bands were simulated, fabricated, and analyzed in terms of manufacturing quality and radio frequency (RF) performance. Samples were manufactured using a 3D printer and PREPERM® ABS1000 filament, which offers a stable dielectric constant (εr = 10 ± 0.35) and low losses (tan δ = 0.003) over wide frequency and temperature ranges. Surface profile tests and microscope measurements revealed discrepancies in the dimensions in the xy-plane and along the z-axis, consistent with the observed shift in resonant frequency. Despite these variations, reasonably good agreement between RF-simulated and measured results was achieved, and the DRA array successfully covered the intended mmWave band. However, challenges in achieving high precision may restrict applications at higher mmWave bands. Nevertheless, compared with conventional methods, FDM techniques offer a highly accessible and flexible solution with a wide range of materials for home and micro-manufacturing of mmWave DRAs for modern 5G systems. Full article
(This article belongs to the Special Issue 5G and Beyond: Technologies and Communications)
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<p>Configuration of the FDM printed microwave DRA: (<b>a</b>) DRA on top of a metallic ground plane, (<b>b</b>) substrate and DRA made transparent to show the microstrip transmission line on the back of the substrate and the slot on the top ground plane.</p>
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<p>Zoom-in view of the top and bottom surfaces of the FDM-printed microwave DRA. (<b>a</b>) top view, (<b>b</b>) bottom view.</p>
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<p>2D cut surface profile of the FDM-printed DRA.</p>
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<p>3D side view and 2D cut surface profile of the FDM-printed DRA.</p>
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<p>Fabricated DRA. (<b>a</b>) top view, (<b>b</b>) bottom view.</p>
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<p>Simulated and measured <span class="html-italic">S</span><sub>11</sub> of the microwave DRA design. Adjusted dimensional parameters and permittivity were also taken into account based on the measured values.</p>
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<p>Configuration of the mmWave DRA array.</p>
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<p>Simulated efficiency and realized gain for mmWave DRA array.</p>
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<p>Beam scanning performance of the DRA array in (<b>a</b>) xz- and (<b>b</b>) yz-plane.</p>
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<p>Gain at broadside direction with different (<b>a</b>) radius, (<b>b</b>) height, (<b>c</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>ε</mi> </mrow> <mrow> <mi>r</mi> </mrow> </msub> </mrow> </semantics></math>, (<b>d</b>) tan <span class="html-italic">δ</span> of DRA element.</p>
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<p>Efficiency with different (<b>a</b>) radius, (<b>b</b>) height, (<b>c</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>ε</mi> </mrow> <mrow> <mi>r</mi> </mrow> </msub> </mrow> </semantics></math>, (<b>d</b>) tan <span class="html-italic">δ</span> of DRA element.</p>
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<p>Configuration of the DRA array with an in-phase feeding network.</p>
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<p>Photographs of the FDM 3D-printed DRA array with an in-phase feeding network. (<b>a</b>) top view, (<b>b</b>) bottom view.</p>
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<p>Zoom-in view of the top and bottom surfaces of the FDM 3D-printed mmWave DRA. (<b>a</b>) top view, (<b>b</b>) bottom view.</p>
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<p>2D cut surface profile of the FDM-printed mmWave DRA.</p>
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<p>3D side view and 2D cut surface profile of the FDM-printed mmWave DRA element.</p>
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<p>Simulated and measured matching performance of the FDM 3D-printed DRA array with in-phase feeding network.</p>
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<p>Simulated and measured radiation patterns of the FDM 3D-printed DRA array at 26.8 GHz. (<b>a</b>) xz- and (<b>b</b>) yz-plane.</p>
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<p>Simulated and measured realized gain at the broadside direction of the FDM 3D-printed DRA array.</p>
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<p>(<b>a</b>) Configuration of the DRA array, and (<b>b</b>) simulated efficiency and realized gain.</p>
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<p>Beam scanning performance of the cuboid DRA array in the (<b>a</b>) xz-, and (<b>b</b>) yz-planes.</p>
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<p>Top view of the FDM 3D-printed cuboid DRA element (<b>a</b>) before, and (<b>b</b>) after refining.</p>
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<p>Side view of the FDM 3D-printed cuboid DRA element (<b>a</b>) before, and (<b>b</b>) after refining.</p>
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12 pages, 17759 KiB  
Article
Attention-Enhanced Defensive Distillation Network for Channel Estimation in V2X mm-Wave Secure Communication
by Xingyu Qi, Yuanjian Liu and Yingchun Ye
Sensors 2024, 24(19), 6464; https://doi.org/10.3390/s24196464 - 7 Oct 2024
Viewed by 817
Abstract
Millimeter-wave (mm-wave) technology, crucial for future networks and vehicle-to-everything (V2X) communication in intelligent transportation, offers high data rates and bandwidth but is vulnerable to adversarial attacks, like interference and eavesdropping. It is crucial to protect V2X mm-wave communication from cybersecurity attacks, as traditional [...] Read more.
Millimeter-wave (mm-wave) technology, crucial for future networks and vehicle-to-everything (V2X) communication in intelligent transportation, offers high data rates and bandwidth but is vulnerable to adversarial attacks, like interference and eavesdropping. It is crucial to protect V2X mm-wave communication from cybersecurity attacks, as traditional security measures often fail to counter sophisticated threats and complex attacks. To tackle these difficulties, the current study introduces an attention-enhanced defensive distillation network (AEDDN) to improve robustness and accuracy in V2X mm-wave communication under adversarial attacks. The AEDDN model combines the transformer algorithm with defensive distillation, leveraging the transformer’s attention mechanism to focus on critical channel features and adapt to complex conditions. This helps mitigate adversarial examples by filtering misleading data. Defensive distillation further strengthens the model by smoothing decision boundaries, making it less sensitive to small perturbations. To evaluate and validate the AEDDN model, this study uses a publicly available dataset called 6g-channel-estimation and a proprietary dataset named MMMC, comparing the simulation results with the convolutional neural network (CNN) model. The findings from the experiments indicate that the AEDDN, especially in the complex V2X mm-wave environment, demonstrates enhanced performance. Full article
(This article belongs to the Special Issue AI-Driven Cybersecurity in IoT-Based Systems)
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<p>Structure of AEDDN algorithm.</p>
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<p>The scenario in the WI simulation platform. (<b>a</b>) Specific trajectories of vehicles. (<b>b</b>) Heat maps and propagation paths.</p>
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<p>Training history for CNN-based and AEDDN models through 6g-channel-estimation dataset. (<b>a</b>) Teacher model training. (<b>b</b>) Student model training.</p>
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<p>Comparative performance of CNN and AEDDN models under adversarial attacks. (<b>a</b>) MSE and ASR comparison under FGSM attack. (<b>b</b>) MSE and ASR comparison under PGD attack.</p>
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<p>Comparison of pilot signals, actual channel, and predicted channel using AEDDN model for MMMC dataset.</p>
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<p>Loss value comparison between CNN-based and AEDDN models through MMMC dataset. (<b>a</b>) Loss value from teacher training and validation. (<b>b</b>) Loss value from student training and validation.</p>
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19 pages, 564 KiB  
Article
Joint Power Allocation and Hybrid Beamforming for Cell-Free mmWave Multiple-Input Multiple-Output with Statistical Channel State Information
by Jiawei Bai, Guangying Wang, Ming Wang and Jinjin Zhu
Sensors 2024, 24(19), 6276; https://doi.org/10.3390/s24196276 - 27 Sep 2024
Viewed by 555
Abstract
Cell-free millimeter wave (mmWave) multiple-input multiple-output (MIMO) can effectively overcome the shadow fading effect and provide macro gain to boost the throughput of communication networks. Nevertheless, the majority of the existing studies have overlooked the user-centric characteristics and practical fronthaul capacity limitations. To [...] Read more.
Cell-free millimeter wave (mmWave) multiple-input multiple-output (MIMO) can effectively overcome the shadow fading effect and provide macro gain to boost the throughput of communication networks. Nevertheless, the majority of the existing studies have overlooked the user-centric characteristics and practical fronthaul capacity limitations. To solve these practical problems, we introduce a resource allocation scheme using statistical channel state information (CSI) for uplink user-centric cell-free mmWave MIMO system. The hybrid beamforming (HBF) architecture is deployed at each access point (AP), while the central processing unit (CPU) only combines the received signals by the large-scale fading decoding (LSFD) method. We further frame the issue of maximizing sum-rate subject to the fronthaul capacity constraint and minimum rate constraint. Based on the alternating optimization (AO) and fractional programming method, we present an algorithm aimed at optimizing the users’ transmit power for the power allocation (PA) subproblem. Then, an algorithm relying on the majorization–minimization (MM) method is given for the HBF subproblem, which jointly optimizes the HBF and the LSFD coefficients. Full article
(This article belongs to the Section Communications)
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<p>Cell-free mmWave MIMO system.</p>
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<p>Hybrid beamforming structure at each AP.</p>
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<p>Sum-rate of system under different power allocation schemes.</p>
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<p>Sum-rate of system under different beamforming schemes.</p>
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<p>Sum-rate of system under different parameters.</p>
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<p>Sum-rate of system with different maximum fronthaul capacity.</p>
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<p>Sum-rate of system with different numbers of APs and antennae.</p>
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<p>Sum-rate of system under different minimum rate.</p>
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40 pages, 4416 KiB  
Review
A Review on Millimeter-Wave Hybrid Beamforming for Wireless Intelligent Transport Systems
by Waleed Shahjehan, Rajkumar Singh Rathore, Syed Waqar Shah, Mohammad Aljaidi, Ali Safaa Sadiq and Omprakash Kaiwartya
Future Internet 2024, 16(9), 337; https://doi.org/10.3390/fi16090337 - 14 Sep 2024
Viewed by 4238
Abstract
As the world braces for an era of ubiquitous and seamless connectivity, hybrid beamforming stands out as a beacon guiding the evolutionary path of wireless communication technologies. Several hybrid beamforming technologies are explored for millimeter-wave multiple-input multi-output (MIMO) communication. The aim is to [...] Read more.
As the world braces for an era of ubiquitous and seamless connectivity, hybrid beamforming stands out as a beacon guiding the evolutionary path of wireless communication technologies. Several hybrid beamforming technologies are explored for millimeter-wave multiple-input multi-output (MIMO) communication. The aim is to provide a roadmap for hybrid beamforming that enhances wireless fidelity. In this systematic review, a detailed literature review of algorithms/techniques used in hybrid beamforming along with performance metrics, characteristics, limitations, as well as performance evaluations are provided to enable communication compatible with modern Wireless Intelligent Transport Systems (WITSs). Further, an in-depth analysis of the mmWave hybrid beamforming landscape is provided based on user, link, band, scattering, structure, duplex, carrier, network, applications, codebook, and reflecting intelligent surfaces to optimize system design and performance across diversified user scenarios. Furthermore, the current research trends for hybrid beamforming are provided to enable the development of advanced wireless communication systems with optimized performance and efficiency. Finally, challenges, solutions, and future research directions are provided so that this systematic review can serve as a touchstone for academics and industry professionals alike. The systematic review aims to equip researchers with a deep understanding of the current state of the art and thereby enable the development of next-generation communication in WITSs that are not only adept at coping with contemporary demands but are also future-proofed to assimilate upcoming trends and innovations. Full article
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<p>Intelligent Transportation Systems (ITSs): the integration of satellite communication, millimeter-wave (mmWave) roadside units, and connected vehicles.</p>
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<p>MmWave-unmanned aerial vehicle (UAV) communications with scenarios such as aerial photography, surveillance, and remote sensing.</p>
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<p>Organization of the systematic review.</p>
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<p>In-depth analysis of Mm-wave hybrid beamforming landscape.</p>
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<p>Hybrid architecture with amplifiers [<a href="#B45-futureinternet-16-00337" class="html-bibr">45</a>].</p>
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<p>Subarray architecture [<a href="#B49-futureinternet-16-00337" class="html-bibr">49</a>,<a href="#B50-futureinternet-16-00337" class="html-bibr">50</a>].</p>
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<p>Muti-group hybrid beamforming design [<a href="#B60-futureinternet-16-00337" class="html-bibr">60</a>].</p>
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<p>Double analog combiner with low-resolution ADCs [<a href="#B62-futureinternet-16-00337" class="html-bibr">62</a>].</p>
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<p>Hybrid architecture [<a href="#B63-futureinternet-16-00337" class="html-bibr">63</a>].</p>
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<p>Subconnected architecture with switches [<a href="#B64-futureinternet-16-00337" class="html-bibr">64</a>].</p>
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<p>Fully connected architecture [<a href="#B64-futureinternet-16-00337" class="html-bibr">64</a>].</p>
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<p>Current trends in Mw-wave hybrid beamforming field.</p>
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<p>Challenges, solutions, and future research directions in Mw-wave hybrid beamforming field.</p>
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13 pages, 373 KiB  
Article
Ambient Backscatter-Based User Cooperation for mmWave Wireless-Powered Communication Networks with Lens Antenna Arrays
by Rongbin Guo, Rui Yin, Guan Wang, Congyuan Xu and Jiantao Yuan
Electronics 2024, 13(17), 3485; https://doi.org/10.3390/electronics13173485 - 2 Sep 2024
Viewed by 532
Abstract
With the rapid consumer adoption of mobile devices such as tablets and smart phones, tele-traffic has experienced a tremendous growth, making low-power technologies highly desirable for future communication networks. In this paper, we consider an ambient backscatter (AB)-based user cooperation (UC) scheme for [...] Read more.
With the rapid consumer adoption of mobile devices such as tablets and smart phones, tele-traffic has experienced a tremendous growth, making low-power technologies highly desirable for future communication networks. In this paper, we consider an ambient backscatter (AB)-based user cooperation (UC) scheme for mmWave wireless-powered communication networks (WPCNs) with lens antenna arrays. Firstly, we formulate an optimization problem to maximize the minimum rate of two users by jointly designing power and time allocation. Then, we introduce auxiliary variables and transform the original problem into a convex form. Finally, we propose an efficient algorithm to solve the transformed problem. Simulation results demonstrate that the proposed AB-based UC scheme outperforms the competing schemes, thus improving the fairness performance of throughput in WPCNs. Full article
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<p>System model and transmission protocol for UC.</p>
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<p>Performance of different schemes.</p>
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<p>Performance of different schemes.</p>
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<p>Performance of different schemes.</p>
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<p>Performance of different schemes.</p>
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