2D MoS2/graphene composites with excellent full Ku band microwave absorption

RSC Advances ◽  
2016 ◽  
Vol 6 (108) ◽  
pp. 106187-106193 ◽  
Author(s):  
Xiaoxia Wang ◽  
Wenling Zhang ◽  
Xuqiang Ji ◽  
Baoqin Zhang ◽  
Mingxun Yu ◽  
...  

2D MoS2/graphene composites were proved to be promising full Ku band MA materials due to their superb high dielectric loss.

2020 ◽  
Vol 31 (9) ◽  
pp. 6843-6854 ◽  
Author(s):  
Tongguang Zhu ◽  
Yong Sun ◽  
Yajing Wang ◽  
Hongna Xing ◽  
Xinyuan Li ◽  
...  

2013 ◽  
Vol 39 (6) ◽  
pp. 7241-7246 ◽  
Author(s):  
Jie Yuan ◽  
Zhi-Ling Hou ◽  
Hui-Jing Yang ◽  
Yong Li ◽  
Yu-Qing Kang ◽  
...  

2001 ◽  
Vol 259 (1) ◽  
pp. 55-60 ◽  
Author(s):  
Chen Xiaogang ◽  
Yao Xi ◽  
Zhang Desheng ◽  
Zhang Liangying

NANO ◽  
2020 ◽  
Vol 15 (08) ◽  
pp. 2050104
Author(s):  
Ying Meng ◽  
Shibin Lu ◽  
Yaodong Wu ◽  
Zhenfa Zi ◽  
Yuan Ma ◽  
...  

In this study, we have successfully synthesized porous CoO–Co@RGO composites using GO and Co-based metal-organic frameworks (MOFs) as precursors. Due to particular structures and advantageous characteristics, the synthesized porous CoO–Co@RGO composites exhibit outstanding electromagnetic (EM) wave absorbing properties with a filler loading of 10[Formula: see text]wt.% in wax matrix. The maximum reflection loss (RL) of the prepared porous CoO–Co@RGO was [Formula: see text][Formula: see text]dB with 2.1[Formula: see text]mm thickness, and the effective absorption bandwidth as wide as 6.24[Formula: see text]GHz (11.76–18[Formula: see text]GHz), which covers the full Ku-band. Remarkably, the achieved all values of[Formula: see text]RL were under [Formula: see text][Formula: see text]dB with 1.0–5.0[Formula: see text]mm thickness, the corresponding to bandwidth range can be tuned to 13.84[Formula: see text]GHz (4.16–18[Formula: see text]GHz). The superior absorbing performance is attributed to suitable magnetic loss, high dielectric loss and large attenuation mainly caused by conduction loss and polarization relaxation.


1998 ◽  
Vol 84 (11) ◽  
pp. 6109-6113 ◽  
Author(s):  
S. L. Browning ◽  
J. Lodge ◽  
R. R. Price ◽  
J. Schelleng ◽  
P. E. Schoen ◽  
...  

2006 ◽  
Vol 88 (21) ◽  
pp. 214103 ◽  
Author(s):  
U. Brohede ◽  
M. Strømme

1996 ◽  
Vol 118 (2) ◽  
pp. 173-188 ◽  
Author(s):  
Minoru Sueki ◽  
George A. Rinard ◽  
Sandra S. Eaton ◽  
Gareth R. Eaton

2021 ◽  
Vol 6 (1) ◽  
pp. 31-35
Author(s):  
Nurul Ainon Bakar ◽  
Muhammad Azwadi Sulaiman ◽  
Julie Juliewatty Mohamed

Nickel oxide (NiO) belongs to the transition metal oxide family, having good dielectric constantwith the range of 103 – 105, but it has high dielectric loss. In this research, the effect of titaniumdioxide (TiO2) addition into NiO was investigated. Generally, TiO2 was used in the application ofelectrical ceramic, catalysts, electric conductors and chemical intermediates. Ni1-xTixO1+x wasprepared via solid-state reaction method with 6 different TiO2 compositions. The preparation startedwith the powder mixing process for 24 hours and followed by calcination process at 950 °C for 4hours. Then, the calcined powders were compacted into 6 mm pellet shape under pressure of 250MPa pressure. Three pellets were made for each TiO2 composition. Those pellets were sintered at1250 °C for 5 hours. XRD results showed that pure NiO at 0.01 and 0.02 mole % of TiO2compositions produced single NiO crystalline phase, while 0.03, 0.05 and 0.10 mol % of TiO2showed the TiO2, instead of NiO phases. SEM analysis showed that increasing TiO2 concentrationmake the grain size increase, with 0.02 mole % of TiO2 gave the largest grain size, shows that 0.02mole % is the optimum TiO2 concentration for grain size enlargement. Furthermore, the bulkdensity of Ni1xTixO1+xpellet was reduces at higher TiO2 concentration. In dielectric test, the additionof 0.03 mole % of TiO2 gave the highest dielectric constant with value of 4.51 x 1014 and 0.05 mole% of TiO2 gives the result of lowest dielectric loss (0.53).


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