Abstract
We theoretically investigate tunable optical absorption properties of photonic crystals containing lossy materials as defects. It is found that a lossy defect can induce one or multiple perfect absorption peaks in the bandgap of photonic crystals and the number of the peaks mainly depends on the thickness of the defect layer. On the one hand, multiple complete absorption peaks can also emerge in the photonic bandgap when multiple lossy defects are inserted within the photonic crystals, and the resonant wavelengths of absorption peaks can be modulated by changing the distances among the defects. On the other hand, the optical absorption away from resonant wavelengths is nearly zero in the whole visible range. Such nanostructures can be used to engineer novel optical devices such as tunable single-channel and multi-channel perfect optical absorbers.
1 Introduction
The media, which can absorb the optical waves strongly, have many important applications, such as photovoltaics, sensors, photodetectors, and imaging [1–7]. Conventional optical absorbers based on bulk materials generally have some shortcomings including fixed material parameters, untunable absorption frequency, and absorption band, which restrict their applications. In recent years, artificial nanostructures attract much attention due to their advantages in realizing tunable optical absorption, where a typical nanostructure is a photonic crystal [6, 7].
Photonic crystals (PCs) are composed of periodic arrangements of materials with different refractive indices, which can be divided into one-dimensional (1D), two-dimensional (2D), or three-dimensional (3D) PCs. Periodic PCs have the photonic bandgap (which can also be called as photonic forbidden gap) so that they can also be named photonic bandgap materials. If defects are inserted into the PCs, defect modes (also named cavity modes) will appear in the photonic bandgap which can induce strong photonic localization [8–11]. On the other hand, the interface mode can also induce photonic localization with special nanostructures, such as photonic heterostructures composed of truncated PCs and thick metallic films [12–15], or different PCs [16]. The enhanced optical absorption can be realized based on the photonic localization in 1D nanostructures [12, 14, 15, 17]. In addition, many 2D and 3D nanostructures are also used to enhance optical absorption such as periodic air holes [18], elliptical nano-disk arrays [19], and metal nanocavity arrays [20]. Compared with 2D and 3D nanostructures, 1D PCs are simpler in the spatial dimension and easier to prepare, so many research works focus on modulating optical properties by 1D nanostructures [21–26] including enhancing optical absorption in PCs containing different defects [26–28]. Currently, the study of perfect absorption in a super wide band is less. In this study, we theoretically demonstrate that single-channel and multi-channel perfect optical absorption can be realized in 1D PCs containing one or multiple lossy defects in the whole visible region which is much larger than the photonic bandgap.
The study is organized as follows. Section 2 describes the tunable optical absorption properties of 1D PCs containing a lossy defect layer. Section 3 describes the tunable optical absorption properties of 1D PCs with multiple lossy defect layers. Finally, the conclusions are drawn in Section 4.
2 Tunable absorption properties of 1D PCs containing a lossy defect layer
In this section, 1D PC containing a lossy defect layer is considered, which is denoted by (AB)MD(BA)N as is shown in Figure 1, where A and B denote TiO2 and SiO2 with refractive indices of nA = 2.123 and nB = 1.431, respectively [29, 30]. M and N represent periodic numbers of the optical barriers on both sides of defect layer D, respectively. For simplicity, the real part of the refractive index for the lossy defect layer D is identical to that of A, and the imaginary part of its refractive index is denoted by kD. The thicknesses of A and B are kept with dA = 66.24Â nm and dB = 98.27 nm, respectively. The thickness of lossy layer D is changed to modulate the absorption properties of the defective PCs.
FIGURE 1
Based on the transfer matrix method [31], Figure 2A shows the simulated absorption spectra of symmetrical PC (AB)5D (BA)5 with kD = 0.006 and dD = 138.28Â nm in the case of normal incidence. It can be seen that the maximum absorptance at the resonant wavelength of 570.65Â nm is nearly 0.5. However, the asymmetrical nanostructures are easier to realize complete absorption [32, 33]. Therefore, we select the asymmetrical PC (AB)MD(BA)N to enhance the optical absorption in this study, the thickness of the defect layer D of which is fixed and the periodic number N is larger than M. Figure 2B shows that there is a perfect absorption peak at the wavelength of 570.58Â nm in the whole visible region for asymmetrical PC (AB)5D(BA)20 with kD = 0.006 and dD = 138.28Â nm. Moreover, by increasing the thickness of defect layer D to dD = 331.86 nm, two perfect absorption peaks at resonant wavelengths of 510.77 nm and 627.06Â nm are obtained in the visible region as described in Figure 2C. It is worth noting that the photonic bandgap of the periodic PC (AB)N is from 499.35 nm to 643.74 nm, which is much narrower than the whole visible region. Therefore, the whole visible range can be regarded as a super wide band. Moreover, for the PC with a thicker defect layer, more perfect absorption peaks can be obtained in the visible region. The reason is that thicker lossy defect as the resonant cavity can induce more resonances in the photonic bandgap of the PC.
FIGURE 2
To understand the physical mechanism of the enhanced absorption more clearly, the electric field intensities in different PCs at defect wavelengths are shown in Figure 3, where the blue and red lines denote the intensities of symmetrical PC (AB)5D(BA)5Â at the wavelength of 570.65Â nm and asymmetrical nanostructure (AB)5D(BA)20Â at the wavelength of 570.58 nm, respectively. (AB)5D(BA)20 has larger intensities than those in the former symmetrical PC so it has perfect absorption at the defect wavelength. The reason is that the absorptance is proportional to the electric field intensities in the lossy defect [14]. Moreover, the electric field intensities of (AB)5D(BA)20 with dD = 331.86Â nm at the wavelengths of 510.77 nm and 627.06Â nm are given in Figure 4A and 4B, respectively. It can be seen that the electric fields are mainly localized within lossy defect layer D.
FIGURE 3
FIGURE 4
Furthermore, the oblique incidence and different polarizations are taken into consideration. The absorption spectra of asymmetrical PCs (AB)5D(BA)20 with different thicknesses of dD = 138.28Â nm and dD = 331.86Â nm are simulated in detail, as shown in Figure 5 and Figure 6, respectively. It can be found that the wavelengths of absorption peaks are blueshift with the increase of incident angle for both polarizations. Importantly, the values of absorption peaks for two different PCs are close to the unit, and those away from absorption wavelengths remain at a low level in a wide range of incidence and in broadband including photonic bandgap and passband, where the variation trends of two band edges with the incident angles are described by yellow lines in Figure 5. Therefore, these asymmetrical defective PCs can be used to fabricate single and multi-channel perfect absorbers in an ultrawide band.
FIGURE 5
FIGURE 6
3 Tunable absorption properties of 1D PCs containing multiple lossy defect layers
In addition to changing the thickness of a defect layer in the PC to realize multiple absorptions, the same effect can also be obtained by inserting multiple lossy defect layers within the PC. In addition, the absorption wavelengths can be modulated by altering the distances among the defect layers. Herein, the asymmetrical PCs containing multiple defect layers are considered. First, the absorption properties of the PCs (AB)5D(BA)ND(AB)20 and (AB)5D(BA)ND(AB)ND(BA)20 are investigated by changing the periodic number N, as shown in Figure 7 and Figure 8, respectively. As shown in Figure 7, two perfect absorption peaks appear in the whole visible range for (AB)5D(BA)ND(AB)20 with kD = 0.0036 and dD = 128.5Â nm. It can be seen that the gap between two absorption wavelengths tends to diminish when the periodic number becomes larger from N = 2 to N = 6. The reason is that the coupling effect between defect modes is stronger when the periodic number N is two rather than four or six [33]. A strong coupling effect can induce large splitting of the defect modes which is inversely proportional to the distance between the defect layers. In Figure 8, three perfect absorption peaks are obtained in the whole visible range for (AB)5D(BA)ND(AB)ND(BA)20 with kD = 0.0023 and dD = 130.3Â nm. It is also found that the spacing among three absorption wavelengths becomes smaller with the increase of the periodic numbers from N = 2 to N = 6. Moreover, if more defect layers are inserted into the PCs, more perfect absorption peaks will be realized in the whole visible region. Therefore, such nanostructures are potential candidates for engineering tunable multi-channel perfect absorbers in the visible range.
FIGURE 7
FIGURE 8
At last, the influence of incident angles and polarizations on the absorption properties of PCs containing multiple defect layers has been studied. For simplicity, two PCs (AB)5D(BA)2D(AB)20 and (AB)5D(BA)2D(AB)2D(BA)20 are the same as those corresponding to Figure 7A and Figure 8A, respectively. In Figure 9 and Figure 10, the wavelengths of absorption peaks are blueshift with increase of the incident angles for TE and TM polarizations. In particular, the absorptance of all peaks remains nearly the unit in a wide range of incident angles, while the absorptances away from the defect wavelengths are very low in the whole visible region.
FIGURE 9
FIGURE 10
4 Conclusion
In summary, we have theoretically demonstrated that optical waves at defect wavelengths can be absorbed completely in asymmetrical PCs with lossy or multiple lossy defects. One or multiple perfect absorption peaks appear in the whole visible region. The number of absorption peaks can be modulated by changing the thickness of the defect layer or the defect number. Moreover, the distances among absorption wavelengths for PCs containing multiple defects can be tuned by altering the distances among the defects. These types of PCs with lossy defects will play an important role in modulating perfect optical absorption in the visible region.
Statements
Data availability statement
The original contributions presented in the study are included in the article/Supplementary Material; further inquiries can be directed to the corresponding author.
Author contributions
GD designed the research. RY, JL, HZ, and YZ performed the research and analyzed the data. GD, RY, and JL wrote the manuscript. GD, FL, and AW contributed to the revisions.
Funding
This research was funded by the Natural Science Foundation of Shandong Province (No. ZR2019MA055).
Conflict of interest
The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.
Publisher’s note
All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors, and the reviewers. Any product that may be evaluated in this article, or claim that may be made by its manufacturer, is not guaranteed or endorsed by the publisher.
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Summary
Keywords
photonic crystals, photonic bandgap, optical absorption, photonic localization, defect modes
Citation
Yan R, Li J, Zhou H, Zhao Y, Liu F, Wu A and Du G (2022) Tunable perfect optical absorption in truncated photonic crystals with lossy defects. Front. Phys. 10:1019214. doi: 10.3389/fphy.2022.1019214
Received
14 August 2022
Accepted
26 August 2022
Published
19 September 2022
Volume
10 - 2022
Edited by
Zhiwei Guo, Tongji University, China
Reviewed by
Junjie Du, East China Normal University, China
Neng Wang, Shenzhen University, China
Updates
Copyright
© 2022 Yan, Li, Zhou, Zhao, Liu, Wu and Du.
This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.
*Correspondence: Guiqiang Du, dgqql@sdu.edu.cn
This article was submitted to Optics and Photonics, a section of the journal Frontiers in Physics
Disclaimer
All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors and the reviewers. Any product that may be evaluated in this article or claim that may be made by its manufacturer is not guaranteed or endorsed by the publisher.