Research Article | | Peer-Reviewed

Versatile Protrusive VO2 Metamaterials Enabling Tunable Ultra-broadband Terahertz Absorption

Published in Optics (Volume 13, Issue 2)
Received: 1 August 2025     Accepted: 15 August 2025     Published: 8 September 2025
Views:       Downloads:
Abstract

Until now, it has been conventional to design tunable metamaterial absorbers with single layer scheme of metal-dielectric-VO2. For further expansion of the operating bandwidth, the construction method stacking several layers of dielctric-VO2 has been utilized. However, the single layer configuration of metal-dielectric-VO2 cannot extend the absorption bandwidth to the entire THz band. Meanwhile, In the stacking method, other VO2 resonators excepting the topmost VO2 resonator are embedded in the dielectric substrate. This unavoidably leads to the delay in response time to external stimuli. So, apart from these conventional methods, we have conceived the protrusive VO2 metamaterials, which are effective for overcoming the above limitations. The protrusive VO2 metamaterials consist of a VO2 square ring, a protrusive VO2 square patch and a polyimide substrate backed with a gold bottom plane. Based on the proposed design idea, we demonstrate a tunable ultra-broadband THz metamaterial absorber (MA) with bandwidth of 9.39 THz. That is, the protrusive VO2 metamaterials greatly enlarge the operating bandwidth with perfect absorption. The proposed MA can obtain the absorptivity above 90% in range of 1.67-11.06 THz, with relative absorption bandwidth of 147.52%. Moreover, the protrusive VO2 metamaterials can realize the absorption tunability by modifying the conductivity of VO2. Additionally, we also demonstrate that the idea of protrusive VO2 metamaterials is very useful for designing several tunable ultra-broadband THz MAs. Owing to the excellent structural versatility, the protrusive VO2 metamaterials are of great value for THz applications.

Published in Optics (Volume 13, Issue 2)
DOI 10.11648/j.optics.20251302.12
Page(s) 24-32
Creative Commons

This is an Open Access article, distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution and reproduction in any medium or format, provided the original work is properly cited.

Copyright

Copyright © The Author(s), 2025. Published by Science Publishing Group

Keywords

Metamaterial Absorber, Versatile, Protrusive, Tunable, Terahertz, Vanadium Dioxide

References
[1] U Nissanov and G Singh Antenna Technology for Terahertz Wireless Communication (Gewerbestrasse: Springer) (2023).
[2] L Guo, X Ma, Z Chang, C Xu, J Liao and R Zhang J. Mater. Res. Technol. 14 772 (2021).
[3] C Caloz, T Itoh and A Rennings IEEE Antennas Propag. Mag. 50 25 (2008).
[4] L Si, K Han, R Niu, L Dong, W Xing and W Zhu Opt. Express 32 19352 (2024).
[5] N I Landy, S Sajuyigbe, J J Mock, D R Smith and W J Padilla Phys. Rev. Lett. 100 207402 (2008).
[6] P T Bowen, A Baron and D R Smith Phys. Rev. A 93 063849 (2016).
[7] X Yang, C Wang, M Qiao and X Li J. Appl. Phys. 137 133104 (2025).
[8] S Sayed, K R Mahmoud and R I Mubarak Sci. Rep. 13 11937 (2023).
[9] S Badri and S Farkoush Appl. Opt. 60 2803 (2021).
[10] N Niharika, S Singh and P. Kumar Optik 253 168551 (2022).
[11] R She, W Liu, Y Lu, Z Zhou and G. Li Appl. Phys. Lett. 115 021101 (2019).
[12] H Zhou, C Yang, D Hu, D Li, X Hui, F Zhang, M Chen and X. Mu Appl. Phys. Lett. 115 143507 (2019).
[13] H Zhu, K Wang, G Liu, J Mou, Y Wu, Z Zhang, Y Qiu and G Wei Opt. Express 30 15939 (2022).
[14] H Tao, N I Landy, C M Bingham, X Zhang, R D Averitt and W J Padilla Opt. Express 16 7181 (2008).
[15] A Faruk and C Sabah Optik 192 162976 (2019).
[16] B X Wang, C Tang, Q S Niu, Y H He and T Chen Nanoscale Res. Lett. 14 64 (2019).
[17] S Asgari and T Fabritius IEEE Access 10 63658 (2022).
[18] S J Guo, C X Hu and H F Zhang J. Opt. Soc. Am. B 37 2678 (2020).
[19] L Liu, W W Liu and Z Y Song J. Appl. Phys. 128 093104 (2020).
[20] M W Jiang, Z Y Song and Q H Liu Opt. Commun. 471 125835 (2020).
[21] R N Dao, X R Kong, H F Zhang and X R Su Optik 180 619 (2019).
[22] L Zheng, R Feng, H Shi and X Li Micromachines 14 1715 (2023).
[23] J N Zhang, G C Wang, B Zhang, T He, Y He and J L Shen Opt. Mater. 54 32 (2016).
[24] M Zhang and Z Y Song Opt. Express 29 21551 (2021).
[25] Z Y Song, K Wang, J W Li and Q H Liu Opt. Express 26 7148 (2018).
[26] Y B Zhang, P H Wu, Z G Zhou, X F Chen, Z Yi, J Y Zhu, T S Zhang and H G Jile IEEE Access 8 85154 (2020).
[27] C Gandhi, P R Babu and K Senthilnathan Front. Optoelectron. 14 288 (2021).
[28] L S Wang, D Y Xia, Q H Fu, X Y Ding and Y Wang Front. Mater. 8 729495 (2021).
[29] Y C Liu, Y X Qian, F R Hu, M Z Jiang and L H Zhang Results Phys. 19 103384 (2020).
[30] Y S Zhou, H Xia, L M Zhang, Y F Zhao and W K Xie Results Phys. 22 103915 (2021).
[31] G S Yang, F P Yan, X M Du, T Li, W Wang, Y L Lv, H Zhou and Y F Hou AIP Adv. 12 045219 (2022).
[32] L Gevorgyan, H Haroyan, H Parsamyan and K Nerkararyan RSC Adv. 13 11948 (2023).
[33] M R Ahmed, O Jyoti, F Farjana, P P Sarkar, A K Paul and M S Habib Opt. Continuum 3 2139 (2024).
[34] M J Yang, U S Jo, M C Ryu, Y G Pak and K J Ri Indian J. Phys. 99 673 (2025).
[35] Y J Wang, Y Y Chen, F Liu, L Chen, K Ji, X C Wang and X L Ji Sci. Rep. 15 10140 (2025).
[36] Y Zhu Mater. Res. Express 12 015801 (2025).
[37] M A Islam, M R Ahmed, O Jyoti, P P Sarkar and M S Habib Opt. Continuum 4 756 (2025).
[38] X F Jiao, Z H Zhang, T Li, Y Xu and G F Song Appl. Sci. 10 7259 (2020).
[39] H L Feng, Z X Zhang, J Y Zhang, D C Fang, J C Wang, et al. Nanomaterials 12 1731 (2022).
[40] K J Ri and C H Ri Opt. Commun. 536 129377 (2023).
[41] K J Ri, J S Kim, J H Kim and C H Ri Opt. Commun. 542 129573 (2023).
[42] S Wang, L Kang and D H Werner Sci. Rep. 7 4326 (2017).
[43] Y Zhao, Q P Huang, H L Cai, X X Lin and Y L Lua Opt. Commun. 426 443 (2018).
[44] X R Kong, H F Zhang, R N Dao and G B Liu J. Electron. Mater. 48 4166-4169 (2019).
[45] A Cavalleri, C Tóth, C W Siders, et al. Phys. Rev. Lett. 87 237401 (2001).
[46] D J Hilton, R P Prasankumar, S Fourmaux, et al. Phys. Rev. Lett. 99 226401 (2007).
[47] Y Xiao, Z H Zhai, Q W Shi, et al. Appl. Phys. Lett. 107 031906 (2015).
Cite This Article
  • APA Style

    Han, Y., Kim, K., Ri, K. (2025). Versatile Protrusive VO2 Metamaterials Enabling Tunable Ultra-broadband Terahertz Absorption. Optics, 13(2), 24-32. https://doi.org/10.11648/j.optics.20251302.12

    Copy | Download

    ACS Style

    Han, Y.; Kim, K.; Ri, K. Versatile Protrusive VO2 Metamaterials Enabling Tunable Ultra-broadband Terahertz Absorption. Optics. 2025, 13(2), 24-32. doi: 10.11648/j.optics.20251302.12

    Copy | Download

    AMA Style

    Han Y, Kim K, Ri K. Versatile Protrusive VO2 Metamaterials Enabling Tunable Ultra-broadband Terahertz Absorption. Optics. 2025;13(2):24-32. doi: 10.11648/j.optics.20251302.12

    Copy | Download

  • @article{10.11648/j.optics.20251302.12,
      author = {Yong-Rok Han and Kwang-Hyok Kim and Kwang-Jin Ri},
      title = {Versatile Protrusive VO2 Metamaterials Enabling Tunable Ultra-broadband Terahertz Absorption
    },
      journal = {Optics},
      volume = {13},
      number = {2},
      pages = {24-32},
      doi = {10.11648/j.optics.20251302.12},
      url = {https://doi.org/10.11648/j.optics.20251302.12},
      eprint = {https://article.sciencepublishinggroup.com/pdf/10.11648.j.optics.20251302.12},
      abstract = {Until now, it has been conventional to design tunable metamaterial absorbers with single layer scheme of metal-dielectric-VO2. For further expansion of the operating bandwidth, the construction method stacking several layers of dielctric-VO2 has been utilized. However, the single layer configuration of metal-dielectric-VO2 cannot extend the absorption bandwidth to the entire THz band. Meanwhile, In the stacking method, other VO2 resonators excepting the topmost VO2 resonator are embedded in the dielectric substrate. This unavoidably leads to the delay in response time to external stimuli. So, apart from these conventional methods, we have conceived the protrusive VO2 metamaterials, which are effective for overcoming the above limitations. The protrusive VO2 metamaterials consist of a VO2 square ring, a protrusive VO2 square patch and a polyimide substrate backed with a gold bottom plane. Based on the proposed design idea, we demonstrate a tunable ultra-broadband THz metamaterial absorber (MA) with bandwidth of 9.39 THz. That is, the protrusive VO2 metamaterials greatly enlarge the operating bandwidth with perfect absorption. The proposed MA can obtain the absorptivity above 90% in range of 1.67-11.06 THz, with relative absorption bandwidth of 147.52%. Moreover, the protrusive VO2 metamaterials can realize the absorption tunability by modifying the conductivity of VO2. Additionally, we also demonstrate that the idea of protrusive VO2 metamaterials is very useful for designing several tunable ultra-broadband THz MAs. Owing to the excellent structural versatility, the protrusive VO2 metamaterials are of great value for THz applications.
    },
     year = {2025}
    }
    

    Copy | Download

  • TY  - JOUR
    T1  - Versatile Protrusive VO2 Metamaterials Enabling Tunable Ultra-broadband Terahertz Absorption
    
    AU  - Yong-Rok Han
    AU  - Kwang-Hyok Kim
    AU  - Kwang-Jin Ri
    Y1  - 2025/09/08
    PY  - 2025
    N1  - https://doi.org/10.11648/j.optics.20251302.12
    DO  - 10.11648/j.optics.20251302.12
    T2  - Optics
    JF  - Optics
    JO  - Optics
    SP  - 24
    EP  - 32
    PB  - Science Publishing Group
    SN  - 2328-7810
    UR  - https://doi.org/10.11648/j.optics.20251302.12
    AB  - Until now, it has been conventional to design tunable metamaterial absorbers with single layer scheme of metal-dielectric-VO2. For further expansion of the operating bandwidth, the construction method stacking several layers of dielctric-VO2 has been utilized. However, the single layer configuration of metal-dielectric-VO2 cannot extend the absorption bandwidth to the entire THz band. Meanwhile, In the stacking method, other VO2 resonators excepting the topmost VO2 resonator are embedded in the dielectric substrate. This unavoidably leads to the delay in response time to external stimuli. So, apart from these conventional methods, we have conceived the protrusive VO2 metamaterials, which are effective for overcoming the above limitations. The protrusive VO2 metamaterials consist of a VO2 square ring, a protrusive VO2 square patch and a polyimide substrate backed with a gold bottom plane. Based on the proposed design idea, we demonstrate a tunable ultra-broadband THz metamaterial absorber (MA) with bandwidth of 9.39 THz. That is, the protrusive VO2 metamaterials greatly enlarge the operating bandwidth with perfect absorption. The proposed MA can obtain the absorptivity above 90% in range of 1.67-11.06 THz, with relative absorption bandwidth of 147.52%. Moreover, the protrusive VO2 metamaterials can realize the absorption tunability by modifying the conductivity of VO2. Additionally, we also demonstrate that the idea of protrusive VO2 metamaterials is very useful for designing several tunable ultra-broadband THz MAs. Owing to the excellent structural versatility, the protrusive VO2 metamaterials are of great value for THz applications.
    
    VL  - 13
    IS  - 2
    ER  - 

    Copy | Download

Author Information
  • Sections