• Photonics Research
  • Vol. 6, Issue 3, 168 (2018)
Amir Ghobadi1、2, Hodjat Hajian1, Alireza Rahimi Rashed1, Bayram Butun1, and Ekmel Ozbay1、2、3、4、*
Author Affiliations
  • 1NANOTAM-Nanotechnology Research Center, Bilkent University, 06800 Ankara, Turkey
  • 2Department of Electrical and Electronics Engineering, Bilkent University, 06800 Ankara, Turkey
  • 3Department of Physics, Bilkent University, 06800 Ankara, Turkey
  • 4UNAM-Institute of Materials Science and Nanotechnology, Bilkent University, 06800 Ankara, Turkey
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    DOI: 10.1364/PRJ.6.000168 Cite this Article Set citation alerts
    Amir Ghobadi, Hodjat Hajian, Alireza Rahimi Rashed, Bayram Butun, Ekmel Ozbay. Tuning the metal filling fraction in metal-insulator-metal ultra-broadband perfect absorbers to maximize the absorption bandwidth[J]. Photonics Research, 2018, 6(3): 168 Copy Citation Text show less

    Abstract

    In this paper, we propose a methodology to maximize the absorption bandwidth of a metal-insulator-metal (MIM) based absorber. The proposed structure is made of a Cr-Al2O3-Cr multilayer design. At the initial step, the optimum MIM planar design is fabricated and optically characterized. The results show absorption above 0.9 from 400 nm to 850 nm. Afterward, the transfer matrix method is used to find the optimal condition for the perfect light absorption in an ultra-broadband frequency range. This modeling approach predicts that changing the filling fraction of the top Cr layer can extend light absorption toward longer wavelengths. We experimentally proved that the use of proper top Cr thickness and annealing temperature leads to a nearly perfect light absorption from 400 nm to 1150 nm, which is much broader than that of a planar design. Therefore, while keeping the overall process lithography-free, the absorption functionality of the design can be significantly improved. The results presented here can serve as a beacon for future performance-enhanced multilayer designs where a simple fabrication step can boost the overall device response without changing its overall thickness and fabrication simplicity.
    Hy(z)={AieikA(zDM1)+AreikA(zDM1),z>DM1M11eikM1z+M12eikM1z,0<z<DM1D1eikIz+D2eikIz,DI<z<0M21eikM2(z+DI)+M22eikM2(z+DI),DIDM2<z<DISteikS[z+(DI+DM2)],z<DIDM2}(1)

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    a=[11ikA/ϵAikA/ϵA],s=[1ikS/ϵS],(2a)

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    m11=[11ikM1/ϵM1ikM1/ϵM1],m12=[eikM1DM1eikM1DM1ikM1eikM1DM1/ϵM1ikM1eikM1DM1/ϵM1],(2b)

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    d1=[11ikI/ϵIikI/ϵI],d2=[eikIDIeikIDIikIeikIDI/ϵIikIeikIDI/ϵI],(2c)

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    m21=[11ikM2/ϵM2ikM2/ϵM2],m22=[eikM2DM2eikM2DM2ikM2eikM2DM2/ϵM2ikM2eikM2DM2/ϵM2],(2d)

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    FFϵMϵeffϵM+ϵeff+(1FF)ϵIϵeffϵI+ϵeff=0,(3)

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    Amir Ghobadi, Hodjat Hajian, Alireza Rahimi Rashed, Bayram Butun, Ekmel Ozbay. Tuning the metal filling fraction in metal-insulator-metal ultra-broadband perfect absorbers to maximize the absorption bandwidth[J]. Photonics Research, 2018, 6(3): 168
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