- Volumes 84-95 (2024)
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Volumes 72-83 (2023)
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Volume 83
Pages 1-258 (December 2023)
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Volume 82
Pages 1-204 (November 2023)
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Volume 81
Pages 1-188 (October 2023)
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Volume 80
Pages 1-202 (September 2023)
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Volume 79
Pages 1-172 (August 2023)
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Volume 78
Pages 1-146 (July 2023)
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Volume 77
Pages 1-152 (June 2023)
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Volume 76
Pages 1-176 (May 2023)
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Volume 75
Pages 1-228 (April 2023)
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Volume 74
Pages 1-200 (March 2023)
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Volume 73
Pages 1-138 (February 2023)
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Volume 72
Pages 1-144 (January 2023)
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Volume 83
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Volumes 60-71 (2022)
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Volume 71
Pages 1-108 (December 2022)
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Volume 70
Pages 1-106 (November 2022)
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Volume 69
Pages 1-122 (October 2022)
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Volume 68
Pages 1-124 (September 2022)
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Volume 67
Pages 1-102 (August 2022)
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Volume 66
Pages 1-112 (July 2022)
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Volume 65
Pages 1-138 (June 2022)
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Volume 64
Pages 1-186 (May 2022)
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Volume 63
Pages 1-124 (April 2022)
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Volume 62
Pages 1-104 (March 2022)
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Volume 61
Pages 1-120 (February 2022)
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Volume 60
Pages 1-124 (January 2022)
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Volume 71
- Volumes 54-59 (2021)
- Volumes 48-53 (2020)
- Volumes 42-47 (2019)
- Volumes 36-41 (2018)
- Volumes 30-35 (2017)
- Volumes 24-29 (2016)
- Volumes 18-23 (2015)
- Volumes 12-17 (2014)
- Volume 11 (2013)
- Volume 10 (2012)
- Volume 9 (2011)
- Volume 8 (2010)
- Volume 7 (2009)
- Volume 6 (2008)
- Volume 5 (2007)
- Volume 4 (2006)
- Volume 3 (2005)
- Volume 2 (2004)
- Volume 1 (2003)
• A new type of bunched CeO2 was prepared by facile hydrothermal method.
• MWCNTs were scattered on surface of bunched CeO2 in CeO2/MWCNTs composite.
• Optimal reflection loss reached −45.72 dB.
• Reflection loss was less than −30 dB in the thickness range of 5.0–7.5 mm at 11.36–17.77 GHz.
A novel bunched cerium oxide (CeO2) was prepared and its binary composite material with multi-walled carbon nanotubes presented an excellent microwave absorbing properties. The morphology, structure, and absorbing properties of the composite material were investigated. It was found that the minimum reflection loss (RL) of the composite material at 15.79 GHz was −45.7 dB when the thickness was 5.5 mm. It was worth noting that when the composite material was in the thickness range of 5.0–7.5 mm and the frequency was 11.36–17.77 GHz, the electromagnetic wave RL was < −30 dB, which illustrated that the composite material had a good absorbing effect over a wide thickness range. The results of the study contributed to the design and preparation of efficient microwave absorbing materials (MAM) with rare earth oxide composites and their applications, which demonstrated the importance of new composites with special structures in the field of MAM.